[0002] The present invention relates to a semiconductor device, which can be used appropriately
as, e.g., a semiconductor device including an insulated gate bipolar transistor (IGBT).
[0003] As an IGBT having a low ON resistance, a trench-gate-type IGBT has been used widely.
There has been developed an IE-type IGBT in which, in a cell formation region, active
cell regions each coupled to an emitter electrode and inactive cell regions each including
a floating region are alternately arranged to allow an IE (Injection Enhancement)
effect to be used. The IE effect reduces the likelihood of discharging of holes from
the emitter electrode when the IGBT is in an ON state and thus increases the density
of the charges stored in a drift region.
[0004] Japanese Unexamined Patent Publication No. 2012-256839 (Patent Document 1) discloses a technique in which, in an IE-type trench-gate IGBT,
each of linear unit cell regions provided in a cell formation region includes a linear
active cell region and linear inactive cell regions provided on both sides of the
linear active cell region such that the linear active cell region is interposed therebetween.
[0005] Japanese Unexamined Patent Publication No. 2013-140885 (Patent Document 2) discloses a technique in which, in an IE-type trench-gate IGBT,
each of linear unit cell regions provided in a cell formation region includes a linear
hybrid cell region and, in the linear hybrid cell region, a first linear hybrid sub-cell
region and a second linear hybrid sub-cell region are provided.
[0006] Japanese Unexamined Patent Publication No. 2006-210547 (Patent Document 3) discloses a technique in which, in an insulated-gate-type semiconductor
device, a second semiconductor layer having a second conductivity type and provided
over a first semiconductor layer having a first conductivity type, a plurality of
striped trenches formed in a top surface of the second semiconductor layer, and a
plurality of third semiconductor regions each having the first conductivity type and
formed selectively in a longitudinal direction between the trenches are provided.
[Related Art Documents]
[Patent Documents]
[0008] There has been known a semiconductor device including an IGBT having a GG-type (gate-gate-type)
active cell region as an IE-type trench-gate IGBT, such as, e.g., the IE-type trench-gate
IGBT disclosed in Patent Document 1 mentioned above. There has also been known a semiconductor
device including an IGBT having an EGE-type (emitter-gate-emitter-type) active cell
region as an IE-type trench gate IGBT, such as, e.g., the IE-type trench-gate IGBT
disclosed in Patent Document 2 mentioned above.
[0009] In the semiconductor device including the IGBT having the EGE-type active region,
in a switching operation when an inductance is coupled as a load, a gate potential
is less affected by a displacement current generated in the active cell region than
in the semiconductor device including the IGBT having the GG-type active cell region.
[0010] However, in the semiconductor device including the IGBT having the EGE-type active
cell region, it is desirable to further improve the performance of the semiconductor
device such as, e.g., the IE effect.
[0011] Other problems and novel features of the present invention will become apparent from
a statement in the present specification and the accompanying drawings.
[0012] According to an embodiment, a semiconductor device includes a first trench gate electrode
and second and third trench gate electrodes located on both sides of the first trench
gate electrode interposed therebetween. The first trench gate electrode is coupled
to a gate electrode. The second and third trench gate electrodes are coupled to an
emitter electrode. In a semiconductor layer between the first and second trench gate
electrodes, a plurality of p
+-type semiconductor regions are formed. In a semiconductor layer between the first
and third trench gate electrodes, a plurality of p
+-type semiconductor regions are formed. Either between the first and second trench
gate electrodes or between the first and third trench gate electrodes, the plurality
of p
+-type semiconductor regions are arranged along an extending direction of the first
trench gate electrode in plan view to be spaced apart from each other.
[0013] According to another embodiment, in a method of manufacturing a semiconductor device,
a first trench gate electrode and second and third trench gate electrodes located
on both sides of the first trench gate electrode interposed therebetween are formed.
The first trench gate electrode is coupled to a gate electrode. The second and third
trench gate electrodes are coupled to an emitter electrode. Next, in a semiconductor
layer between the first and second trench gate electrodes, a plurality of p
+-type semiconductor regions are formed and, in a semiconductor layer between the first
and third trench gate electrodes, a plurality of p
+-type semiconductor regions are formed. Either between the first and second trench
gate electrodes or between the first and third trench gate electrodes, the plurality
of p
+-type semiconductor regions are arranged along an extending direction of the first
trench gate electrode in plan view to be spaced apart from each other.
[0014] According to the embodiment, the performance of the semiconductor device can be improved.
[0015] In the drawings:
FIG. 1 is a plan view of a semiconductor chip as a semiconductor device in Embodiment
1;
FIG. 2 is a main-portion plan view of the semiconductor device in Embodiment 1;
FIG. 3 is a main-portion plan view of the semiconductor device in Embodiment 1;
FIG. 4 is a main-portion cross-sectional view of the semiconductor device in Embodiment
1;
FIG. 5 is a main-portion cross-sectional view of the semiconductor device in Embodiment
1;
FIG. 6 is a main-portion cross-sectional view of the semiconductor device in Embodiment
1;
FIG. 7 is a main-portion cross-sectional view showing the manufacturing process of
the semiconductor device in Embodiment 1;
FIG. 8 is a main-portion cross-sectional view showing the manufacturing process of
the semiconductor device in Embodiment 1;
FIG. 9 is a main-portion cross-sectional view showing the manufacturing process of
the semiconductor device in Embodiment 1;
FIG. 10 is a main-portion cross-sectional view showing the manufacturing process of
the semiconductor device in Embodiment 1;
FIG. 11 is a main-portion cross-sectional view showing the manufacturing process of
the semiconductor device in Embodiment 1;
FIG. 12 is a main-portion cross-sectional view showing the manufacturing process of
the semiconductor device in Embodiment 1;
FIG. 13 is a main-portion cross-sectional view showing the manufacturing process of
the semiconductor device in Embodiment 1;
FIG. 14 is a main-portion cross-sectional view showing the manufacturing process of
the semiconductor device in Embodiment 1;
FIG. 15 is a main-portion cross-sectional view showing the manufacturing process of
the semiconductor device in Embodiment 1;
FIG. 16 is a main-portion cross-sectional view showing the manufacturing process of
the semiconductor device in Embodiment 1;
FIG. 17 is a main-portion cross-sectional view showing the manufacturing process of
the semiconductor device in Embodiment 1;
FIG. 18 is a main-portion cross-sectional view showing the manufacturing process of
the semiconductor device in Embodiment 1;
FIG. 19 is a main-portion cross-sectional view showing the manufacturing process of
the semiconductor device in Embodiment 1;
FIG. 20 is a main-portion cross-sectional view showing the manufacturing process of
the semiconductor device in Embodiment 1;
FIG. 21 is a main-portion cross-sectional view showing the manufacturing process of
the semiconductor device in Embodiment 1;
FIG. 22 is a main-portion cross-sectional view showing the manufacturing process of
the semiconductor device in Embodiment 1;
FIG. 23 is a main-portion cross-sectional view showing the manufacturing process of
the semiconductor device in Embodiment 1;
FIG. 24 is a main-portion cross-sectional view showing the manufacturing process of
the semiconductor device in Embodiment 1;
FIG. 25 is a main-portion cross-sectional view of a semiconductor device in Comparative
Example 1;
FIG. 26 is a main-portion plan view of a semiconductor device in Comparative Example
2;
FIG. 27 is a main-portion plan view of the semiconductor device in Comparative Example
2;
FIG. 28 is a main-portion cross-sectional view of the semiconductor device in Comparative
Example 2;
FIG. 29 is a cross-sectional view showing displacement current paths when the semiconductor
device in Comparative Example 1 is turned ON in overlapping relation;
FIG. 30 is an equivalent circuit diagram showing the displacement current paths when
the semiconductor device in Comparative Example 1 is turned ON;
FIG. 31 is a cross-sectional view showing displacement current paths when the semiconductor
device in Comparative Example 2 is turned ON in overlapping relation;
FIG. 32 is an equivalent circuit diagram showing the displacement current paths when
the semiconductor device in Comparative Example 2 is turned ON;
FIG. 33 is a cross-sectional view showing a p-channel parasitic MOSFET in the semiconductor
device in Comparative Example 2;
FIG. 34 is a circuit diagram showing an equivalent circuit in an L-load switching
test;
FIG. 35 is a view schematically showing a switching waveform in the L-load switching
test;
FIG. 36 is a graph showing a switching waveform when the semiconductor device in Comparative
Example 2 is turned OFF;
FIG. 37 is a graph showing a switching waveform when the semiconductor device in Comparative
Example 2 is turned OFF;
FIG. 38 is a cross-sectional view showing a hole density distribution when the semiconductor
device in Comparative Example 2 is turned OFF;
FIG. 39 is a graph showing the dependence of a collector current on a collector-emitter
voltage in each of the semiconductor devices in Comparative Examples 1 and 2 in an
ON state;
FIG. 40 is a graph showing the dependence of the collector current on the collector-emitter
voltage in each of the semiconductor devices in Comparative Examples 1 and 2 in the
ON state;
FIG. 41 is a graph showing the dependence of the collector current on the collector-emitter
voltage in each of the semiconductor devices in Comparative Examples 1 and 2 in the
ON state;
FIG. 42 is a graph showing a hole density distribution in a thickness direction in
the semiconductor device in Comparative Example 1 in the ON state;
FIG. 43 is a graph showing the hole density distribution in the thickness direction
in the semiconductor device in Comparative Example 1 in the ON state;
FIG. 44 is a graph showing the hole density distribution in the thickness direction
in the semiconductor device in Comparative Example 1 in the ON state;
FIG. 45 is a graph showing a hole density distribution in a thickness direction in
the semiconductor device in Comparative Example 2 in the ON state;
FIG. 46 is a graph showing the hole density distribution in the thickness direction
in the semiconductor device in Comparative Example 2 in the ON state;
FIG. 47 is a graph showing the hole density distribution in the thickness direction
in the semiconductor device in Comparative Example 2 in the ON state;
FIG. 48 is a graph showing a switching waveform when the semiconductor device in Comparative
Example 2 is turned ON;
FIG. 49 is a graph showing a switching waveform when the semiconductor device in Comparative
Example 2 is turned ON;
FIG. 50 is a cross-sectional view showing a hole density distribution in the semiconductor
device in Comparative Example 1 in the ON state;
FIG. 51 is a cross-sectional view showing a hole density distribution in the semiconductor
device in Comparative Example 2 in the ON state;
FIG. 52 is a graph showing the potential dependence of a hole current density when
the semiconductor device in Comparative Example 2 is turned OFF;
FIG. 53 is a graph showing the potential dependence of the hole current density when
the semiconductor device in Comparative Example 2 is turned ON;
FIG. 54 is a circuit block diagram showing an example of an electronic system in which
a semiconductor device in Embodiment 2 is used;
FIG. 55 is an equivalent circuit diagram showing a module as the semiconductor device
in Embodiment 2;
FIG. 56 is a graph showing the gate charge quantity dependence of a gate-emitter voltage
in a semiconductor device in Comparative Example 3;
FIG. 57 is a graph showing the gate charge quantity dependence of a gate-emitter electrode
in the semiconductor device in Embodiment 2;
FIG. 58 is a graph showing switching waveforms when the semiconductor device in Comparative
Example 3 and the semiconductor device in Embodiment 2 are turned OFF by L-load switching;
FIG. 59 is a graph showing switching waveforms when the semiconductor device in Comparative
Example 3 and the semiconductor device in Embodiment 2 are turned OFF by L-load switching;
FIG. 60 is an equivalent circuit diagram showing a pseudo device model of each of
the IGBT chips included in the semiconductor device in Comparative Example 3;
FIG. 61 is an equivalent circuit diagram showing a pseudo device model of each of
the IGBT chips included in the semiconductor device in Embodiment 2;
FIG. 62 is a circuit diagram for circuit simulation in each of the semiconductor devices
in Comparative Example 3 and Embodiment 2;
FIG. 63 is a graph showing the result of the circuit simulation in the semiconductor
device in Comparative Example 3;
FIG. 64 is a graph showing the result of the circuit simulation in the semiconductor
device in Embodiment 2;
FIG. 65 is a main-portion plan view of a semiconductor device in Embodiment 3;
FIG. 66 is a main-portion cross-sectional view of the semiconductor device in Embodiment
3;
FIG. 67 is a main-portion plan view of a semiconductor device in a modification of
Embodiment 3;
FIG. 68 is a main-portion cross-sectional view of the semiconductor device in the
modification of Embodiment 3;
FIG. 69 is a main-portion plan view of a semiconductor device in Embodiment 4;
FIG. 70 is a main-portion cross-sectional view of the semiconductor device in Embodiment
4;
FIG. 71 is a main-portion plan view of a semiconductor device in a modification of
Embodiment 4; and
FIG. 72 is a main-portion cross-sectional view of the semiconductor device in the
modification of Embodiment 4.
[0016] In the following embodiments, if necessary for the sake of convenience, the embodiments
will be each described by being divided into a plurality of sections or embodiments.
However, they are by no means irrelevant to each other unless particularly explicitly
described otherwise, but are in relations such that one of the sections or embodiments
is a modification, details, supplementary explanation, and so forth of part or the
whole of the others.
[0017] Also, in the following embodiments, when the number and the like (including the number,
numerical value, amount, range, and the like) of elements are mentioned, they are
not limited to specific numbers unless particularly explicitly described otherwise
or unless they are obviously limited to specific numbers in principle. The number
and the like of the elements may be not less than or not more than specific numbers.
[0018] Also, in the following embodiments, it goes without saying that the components thereof
(including also elements, steps, and the like) are not necessarily indispensable unless
particularly explicitly described otherwise or unless the components are considered
to be obviously indispensable in principle. Likewise, if the shapes, positional relationships,
and the like of the components and the like are mentioned in the following embodiments,
the shapes and the like are assumed to include those substantially proximate or similar
thereto and the like unless particularly explicitly described otherwise or unless
it can be considered that they obviously do not in principle. The same shall apply
in regard to the foregoing numerical value and range.
[0019] The following will describe representative embodiments in detail on the basis of
the drawings. Note that, throughout all the drawings for illustrating the embodiments,
members having the same functions are designated by the same reference numerals, and
a repeated description thereof is omitted. In the following embodiments, a description
of the same or like parts will not be repeated in principle unless particularly necessary.
[0020] In the drawings used in the embodiments, hatching may be omitted even in a cross
section for improved clarity of illustration, while even a plan view may be hatched
for improved clarity of illustration.
(Embodiment 1)
[0021] A detailed description will be given below of a semiconductor device in Embodiment
1 with reference to the drawings. The semiconductor device in Embodiment 1 includes
an IGBT having an EGE-type (emitter-gate-emitter-type) active cell region. Note that
the possession of the EGE-type active cell region by the IGBT means that, among three
trench gate electrodes arranged in the active cell region to be spaced apart from
each other, the trench gate electrode located in the middle is electrically coupled
to a gate electrode and each of the two trench gate electrodes located at both ends
is electrically coupled to an emitter electrode.
<Configuration of Semiconductor Device>
[0022] First, a description will be given of a configuration of a semiconductor chip as
the semiconductor device in Embodiment 1.
[0023] FIG. 1 is a plan view of the semiconductor chip as the semiconductor device in Embodiment
1. FIGS. 2 and 3 are main-portion plan views of the semiconductor device in Embodiment
1. FIGS. 4 to 6 are main-portion cross-sectional views of the semiconductor device
in Embodiment 1. FIG. 3 shows an area AR3 enclosed by the two-dot-dash line in FIG.
2. FIG. 4 is a cross-sectional view along the line A-A in FIG. 3. FIG. 5 is a cross-sectional
view along the line B-B in FIG. 3. FIG. 6 is a cross-sectional view along the line
C-C in FIG. 3.
[0024] Note that, for easier understanding, FIG. 1 shows the semiconductor device in Embodiment
1 in a see-through state where an insulating film FPF (see FIG. 4) has been removed
and shows the respective outer peripheries of a cell formation area AR1, an emitter
pad EP, and a gate pad GP by the two-dot-dash lines. Also, for easier understanding,
FIG. 2 shows the semiconductor device in Embodiment 1 in a see-through state where
the insulating film FPF, a gate wire GL, an emitter electrode EE, an interlayer insulating
film IL, and the portion of a p-type body region PB (see FIG. 4) which is formed over
a p-type floating region PR have been removed and shows the respective outer peripheries
of the cell formation area AR1 and the gate wire GL by the two-dot-dash lines.
[0025] As shown in FIG. 1, the semiconductor chip CHP as the semiconductor device in Embodiment
1 has a semiconductor substrate SS. The semiconductor substrate has an upper surface
Sa (see FIG. 4) as one main surface and a lower surface Sb (see FIG. 4) as the other
main surface opposite to the upper surface. The semiconductor substrate SS also has
the cell formation area AR1 as a local area of the upper surface Sa and a gate-wire-lead-out
area AR2 as another local area of the upper surface Sa. The gate-wire-lead-out area
AR2 is provided closer to, e.g., the outer periphery of the semiconductor substrate
SS than the cell formation area AR1.
[0026] In the cell formation area AR1, the emitter electrode EE is provided. The center
portion of the emitter electrode EE serves as the emitter pad EP to which bonding
wires or the like are to be coupled. The emitter pad EP is made of the portion of
the emitter electrode EE which is exposed from an opening OP1 formed in the insulating
film FPF (see FIG. 4) formed so as to cover the emitter electrode EE. The emitter
electrode EE is made of a metal film containing, e.g., aluminum as a main component.
[0027] In the gate-wire-lead-out area AR2, the gate wire GL and a gate electrode GE are
provided. The gate wire GL is provided closer to, e.g., the outer periphery of the
semiconductor substrate SS than the emitter electrode EE. The gate wire GL is coupled
to the gate electrode GE. The center portion of the gate electrode GE serves as the
gate pad GP to which bonding wires or the like are to be coupled. The gate pad GP
is made of the portion of the gate electrode GE which is exposed from an opening OP2
formed in the insulating film FPF (see FIG. 4) formed so as to cover the gate electrode
GE. Each of the gate wire GL and the gate electrode GE is made of a metal film containing,
e.g., aluminum as a main component.
[0028] As shown in FIGS. 1 to 6, two directions crossing each other, or preferably orthogonal
to each other in the upper surface of the semiconductor substrate SS are assumed to
be an X-axis direction and a Y-axis direction and a direction perpendicular to the
upper surface of the semiconductor substrate SS, i.e., vertical direction is assumed
to be a Z-axis direction. At this time, in the cell formation area AR1, as shown in
FIG. 2, a plurality of unit cell regions LC are provided. In plan view, the plurality
of unit cell regions LC extend in the Y-axis direction and are periodically arranged
in the X-axis direction.
[0029] Note that, in the present specification, the wording "in plan view" means that an
object is viewed from a direction perpendicular to the upper surface Sa of the semiconductor
substrate SS.
[0030] Each of the unit cell regions LC includes a hybrid cell region LCh as an EGE-type
active cell region and two inactive cell regions LCi. The two inactive cell regions
LCi are located on both sides of the hybrid cell region LCh interposed therebetween
in the X-axis direction. Each of the hybrid cell region LCh and the two inactive cell
regions LCi extends in the Y-axis direction in plan view. Preferably, the hybrid cell
region LCh has a width Wh smaller than a width Wi of each of the inactive cell regions
LCi.
[0031] The two unit cell regions LC adjacent to each other in the X-axis direction share
one of the inactive cell regions LCi. Accordingly, each of the unit cell regions LC
has a positive half portion LCi1 of the inactive cell region LCi which is located
on the negative side of the hybrid cell region LCh in the X-axis direction to be adjacent
thereto. The unit cell region LC also has a negative half portion LCi2 of the inactive
cell region LCi which is located on the positive side of the hybrid cell region LCh
in the X-axis direction to be adjacent thereto.
[0032] The hybrid cell region LCh includes hybrid sub-cell regions LCh1 and LCh2. The hybrid
cell region LCh also includes a trench gate electrode TG1 located at a boundary surface
between the hybrid sub-cell regions LCh1 and LCh2.
[0033] The trench gate electrode TG1 is provided in the middle of the hybrid cell region
LCh. This allows a width Wh1 of the hybrid sub-cell region LCh1 and a width Wh2 of
the hybrid sub-cell region LCh2 to be equal and allows the hybrid sub-cell regions
LCh1 and LCh2 to be arranged symmetrically relative to the trench gate electrode TG1.
[0034] The hybrid cell region LCh has trench gate electrodes TG2 and TG3. The trench gate
electrode TG2 is located between the hybrid sub-cell region LCh1 and the portion LCi1
of the inactive cell region LCi. The trench gate electrode TG3 is located between
the hybrid sub-cell region LCh2 and the portion LCi2 of the inactive cell region LCi.
The trench gate electrodes TG2 and TG3 are electrically coupled to the emitter electrode
EE.
[0035] In the hybrid sub-cell region LCh1, in the portion of the p-type body region PB which
is closer to the upper surface Sa of the semiconductor substrate SS, a plurality of
n
+-type emitter regions NE are formed. The p-type body region PB is a semiconductor
region having a p-type conductivity type. The n
+-type emitter regions NE are semiconductor regions each having an n-type conductivity
type different from the p-type conductivity type. In the hybrid sub-cell region LCh1,
the p-type body region PB is formed continuously along the Y-axis direction in plan
view. In the hybrid sub-cell region LCh1, the plurality of n
+-type emitter regions NE are arranged along the Y-axis direction in plan view to be
spaced apart from each other.
[0036] Note that, in the present specification, the fact that a semiconductor has the p-type
conductivity type means that only holes or both electrons and holes may be charge
carriers, the density of the holes is higher than the density of the electrons, and
the holes are major charge carriers. Also, in the present specification, the fact
that a semiconductor has the n-type conductivity type means that only electrons or
both electrons and holes may be charge carriers, the density of the electrons is higher
than the density of the holes, and the electrons are major charge carriers.
[0037] In the hybrid sub-cell region LCh2, in the portion of the p-type body region BP which
is closer to the upper surface Sa of the semiconductor substrate SS, the plurality
of n
+-type emitter regions NE are provided. In the hybrid sub-cell region LCh2, the p-type
body region PB is formed continuously along the Y-axis direction in plan view. In
the hybrid sub-cell region LCh2, the plurality of n
+-type emitter regions NE are arranged along the Y-axis direction to be spaced apart
from each other.
[0038] In each of the hybrid sub-cell regions LCh1 and LCh2, regions where the n
+-type emitter regions NE are formed along the Y-axis direction, i.e., active sections
LCaa and regions (p-type body region PB) where the n
+-type emitter regions NE are not formed, i.e., inactive sections LCai are alternately
arranged.
[0039] In the inactive cell regions LCi, p-type floating regions PF are provided. The end
portions of the p-type floating regions PF which are closer to the lower surface Sb
are located closer to the lower surface Sb in the Z-axis direction than the end portions
of trenches T1, T2, and T3 which are closer to the lower surface Sb. In the trenches
T1, T2, and T3, the trench gate electrodes TG1, TG2, and TG3 are respectively formed.
In such a case, even when the width Wi of the inactive cell region LCi in the X-axis
direction is larger than the width Wh of the hybrid cell region LCh in the X-axis
direction, a sufficient breakdown voltage can be ensured.
[0040] Note that, in the example shown in FIG. 2, the width Wh of the hybrid cell region
LCh in the X-axis direction is set smaller than the width Wi of each of the inactive
cell regions LCi in the X-axis direction. In such a case, the IE effect of the IGBT
can be enhanced.
[0041] The gate-wire-lead-out area AR2 has a portion where, e.g., a p-type floating region
PFp is provided so as to surround the cell formation area AR1. The p-type floating
region PFp is electrically coupled to the emitter electrode EE via the portion of
a p
+-type body contact region PBCp which is exposed at the bottom surface of a contact
trench CT.
[0042] In the gate-wire-lead-out area AR2, the gate wire GL is placed and the trench gate
electrode TG1 extends from within the cell formation area AR1 toward the gate wire
GL. In the gate-wire-lead-out area AR2, the respective end portions of the adjacent
two trench gate electrodes TG1 are coupled to each other by a trench gate electrode
TGz. In plan view, the trench gate electrode TGz is located in the region where the
gate wire GL is located. The trench gate electrode TGz is electrically coupled to
the gate wire GL via a coupling electrode GTG. Note that the end portion of each of
the inactive cell regions LCi which is closer to the gate-wire-lead-out area AR2 is
defined by an end-portion trench gate electrode TGp.
[0043] In plan view, the trench gate electrodes TG2 and TG3 are located on both sides of
the inactive cell region LCi interposed therebetween. The trench gate electrode TG3
is electrically coupled to the trench gate electrode TG2 not only by the end-portion
trench gate electrode TGp, but also by an emitter coupling portion TGx made of, e.g.,
a polycrystalline silicon film and formed in the same layer as those of the trench
gate electrodes TG2 and TG3. The emitter coupling portion TGx is electrically coupled
to the emitter electrode EE via the contact trench CT formed in the emitter coupling
portion TGx. By thus providing such a structure, it is possible to improve the reliability
of electrical coupling between the trench gate electrodes TG2 and TG3 and the emitter
electrode EE.
[0044] In Embodiment 1, in the hybrid sub-cell region LCh1, a plurality of p
+-type semiconductor regions PR each including a p
+-type body contact region PBC and a p
+-type latch-up preventing region PLP are provided. In the hybrid sub-cell region LCh1,
the plurality of p
+-type semiconductor regions PR are formed in the respective portions of a semiconductor
layer SLn which are located between the trenches T1 and T2 to be in contact with the
p-type body region PB.
[0045] In the hybrid sub-cell region LCh1, the plurality of p
+-type semiconductor regions PR are arranged along the Y-axis direction in plan view
to be spaced apart from each other. This can reduce the ON voltage of the semiconductor
chip CHP and reduce a switching loss when an IGBT in which an inductor having an inductance
L is coupled as a load to a collector electrode or an emitter electrode is subjected
to switching (hereinafter referred to also as "L-load switching") to be turned ON.
[0046] Note that, in the present specification, a switching operation in which the IGBT
shifts from an OFF state to an ON state is referred to as "turn-ON" and a switching
operation in which the IGBT shifts from the ON state to the OFF state is referred
to as "turn-OFF".
[0047] Also, in the hybrid sub-cell region LCh1, in the p-type body region PB, the plurality
of contact trenches CT as openings are formed in the p-type body region PB. The plurality
of contact trenches CT are arranged along the Y-axis direction to be spaced apart
from each other in plan view. The plurality of contact trenches CT reach the p
+-type body contact region PBC located in the hybrid sub-cell region LCh1.
[0048] Also, in Embodiment 1, in the hybrid sub-cell region LCh2, the plurality of p
+-type body contact regions PR each including the p
+-type body contact region PBC and the p
+-type latch-up preventing region PLP are provided. In the hybrid sub-cell region LCh2,
the plurality of p
+-type semiconductor regions PR are formed in the respective portions of the semiconductor
layer SLn which are located between the trenches T1 and T3 to be in contact with the
p-type body region PB.
[0049] In the hybrid sub-cell region LCh2, the plurality of p
+-type semiconductor regions PR are arranged along the Y-axis direction in plan view
to be spaced apart from each other. This can reduce the ON voltage of the semiconductor
chip CHP and reduce the switching loss when the semiconductor chip CHP is turned ON
by the L-load switching.
[0050] Also, in the hybrid sub-cell region LCh2, in the p-type body region PB, the plurality
of contact trenches CT as openings are formed. The plurality of contact trenches CT
are arranged along the Y-axis direction in plan view to be spaced apart from each
other. Each of the plurality of contact trenches CT reaches the p
+-type body contact region PBC located in the hybrid sub-cell region LCh2.
[0051] As shown in FIGS. 2 and 6, in each of the hybrid sub-cell regions LCh1 and LCh2,
the regions where the p
+-type semiconductor regions PR are formed, i.e., active sections LCba and the regions
where the p
+-type semiconductor regions PR are not formed, i.e., inactive sections LCbi are alternately
arranged.
[0052] In Embodiment 1, in the hybrid sub-cell region LCh1, the plurality of n
+-type emitter regions NE are preferably located at the same positions as those of
the plurality of p
+-type semiconductor regions PR in the Y-axis direction. Also, in Embodiment 1, in
the hybrid sub-cell region LCh2, the plurality of n
+-type emitter regions NE are located at the same positions as those of the plurality
of p
+-type semiconductor regions PR in the Y-axis direction.
[0053] Next, a description will be given of a configuration of the unit cell regions LC
in the semiconductor chip as the semiconductor device in Embodiment 1. Specifically,
using FIGS 4 to 6, the description will be given of cross-sectional structures along
the lines A-A, B-B, and C-C in FIG. 3.
[0054] As shown in FIGS. 4 to 6, the semiconductor substrate SS has the upper surface Sa
as the first main surface and the lower surface Sb as the second main surface opposite
to the upper surface Sa. In the semiconductor substrate SS, the n-type semiconductor
layer SLn is formed. In the portion of the semiconductor substrate SS which is located
closer to the lower surface Sb than the semiconductor layer SLn, a semiconductor layer
SLp is formed.
[0055] In the portion of the semiconductor layer SLn other than the upper-layer portion
thereof, an n
--type drift region ND is formed as an n-type semiconductor region. Between the semiconductor
layers SLn and SLp, an n-type field stop region Ns is formed as an n-type semiconductor
region. The semiconductor layer SLp forms a p
+-type collector region CL as a p-type semiconductor region. Over the lower surface
Sb of the semiconductor substrate SS, the collector electrode CE electrically coupled
to the p
+-type collector region CL, i.e., the semiconductor layer SLp is formed.
[0056] On the other hand, in the cell formation area AR1, the p-type body region PB is provided
closer to the upper surface Sa of the semiconductor substrate SS, i.e., in the upper-layer
portion of the semiconductor layer SLn.
[0057] In the upper surface Sa of the semiconductor substrate SS at the boundary portion
between the hybrid sub-cell regions LCh1 and LCh2, the trench T1 is formed as a trench
portion. The trench T1 extends in the Y-axis direction from the upper surface Sa in
plan view to reach a middle point in the semiconductor layer SLn.
[0058] Over the inner wall of the trench T1, the gate insulating film GI is formed. In the
trench T1, the trench gate electrode TG1 is formed over the gate insulating film GI
so as to be embedded in the trench T1. The trench gate electrode TG1 is electrically
coupled to the gate electrode GE (see FIG. 1). Note that the trench gate electrode
TG1 is formed continuously along the Y-axis direction in plan view.
[0059] On the other hand, in the upper surface Sa of the semiconductor substrate SS in the
boundary portion between the hybrid cell region LCh and the inactive cell region LCi,
the trenches T2 and T3 each as the trench portion are formed. Each of the trenches
T2 and T3 extends from the upper surface Sa to reach a middle point in the semiconductor
layer SLn. The trenches T2 and T3 are located on both sides of the trench T1 interposed
therebetween to extend in the Y-axis direction in plan view.
[0060] Over the inner wall of each of the trenches T2 and T3, the gate insulating film GI
is formed. In the trench T2, the trench gate electrode TG2 is formed over the gate
insulating film GI so as to be embedded in the trench T2. In the trench T3, the trench
gate electrode TG3 is formed over the gate insulating film GI so as to be embedded
in the trench T3. The trench gate electrodes TG2 and TG3 are electrically coupled
to the emitter electrode EE. Note that, each of the trench gate electrodes TG2 and
TG3 is formed continuously along the Y-axis direction in plan view.
[0061] In the hybrid sub-cell region LCh1, the p-type body region PB is formed in the portion
of the semiconductor layer SLn which is located between the trenches T1 and T2 to
be in contact with the gate insulating film GI formed over the inner wall of the trench
T1 and with the gate insulating film GI formed over the inner wall of the trench T2.
In the hybrid sub-cell region LCh2, the p-type body region PB is formed in the portion
of the semiconductor layer SLn which is located between the trenches T1 and T3 to
be in contact with the gate insulating film GI formed over the inner wall of the trench
T1 and with the gate insulating film GI formed over the inner wall of the trench T3.
[0062] As shown in FIG. 4, in the cross section along the line A-A in FIG. 3, in each of
the hybrid-sub-cell regions LCh1 and LCh2, the n
+-type emitter region NE is formed only in the portion of the upper surface Sa of the
semiconductor substrate SS which is closer to the trench gate electrode TG1. On the
other hand, as shown in FIG. 5, in the cross section along the line B-B, in each of
the hybrid sub-cell formation regions LCh1 and LCh2, the n
+-type emitter region NE is not formed in the upper surface Sa of the semiconductor
substrate SS.
[0063] As described above, in the hybrid sub-cell region LCH1, the plurality of n
+-type emitter regions NE are arranged along the Y-axis direction in plan view to be
spaced apart from each other. In the hybrid sub-cell region LCh2, the plurality of
n
+-type emitter regions NE are arranged along the Y-axis direction in plan view to be
spaced apart from each other.
[0064] As shown in FIG. 4, in the cross section along the line A-A in FIG. 3, in the hybrid
sub-cell region LCh1, the n
+-type emitter region NE is formed in the portion of the semiconductor layer SLn which
is located between the trenches T1 and T2 to be in contact with the p-type body region
PB and with the gate insulating film GI formed over the inner wall of the trench T1.
On the other hand, in the hybrid sub-cell region LCh2, the n
+-type emitter region NE is formed in the portion of the semiconductor layer SLn which
is located between the trenches T1 and T3 to be in contact with the p-type body region
PB and with the gate insulating film GI formed over the inner wall of the trench T1.
[0065] The plurality of n
+-type emitter regions NE formed in the hybrid sub-cell region LCh1 are electrically
coupled to the emitter electrode EE. The plurality of n
+-type emitter regions NE formed in the hybrid sub-cell region LCh2 are electrically
coupled to the emitter electrode EE.
[0066] Preferably, in each of the hybrid sub-cell regions LCh1 and LCh2, under the p-type
body region PB, an n-type hole barrier region NHB as an n-type semiconductor region
is formed. In each of the hybrid sub-cell regions CLh1 and LCh2, the n-type impurity
concentration in the n-type hole barrier region NHB is higher than the n-type impurity
concentration in the portion of the semiconductor layer SLn (n
--type drift region ND) which is located closer to the lower surface Sb than the n-type
hole barrier region NHB and lower than the n-type impurity concentration in the n
+-type emitter region NE.
[0067] In the hybrid sub-cell region LCh1, the n-type hole barrier region NHB is formed
in the portion of the semiconductor layer SLn which is located between the trenches
T1 and T2. In the hybrid sub-cell region LCh2, the n-type hole barrier region NHB
is formed in the portion of the semiconductor layer SLn which is located between the
trenches T1 and T3.
[0068] Note that, in the hybrid sub-cell region LCh1, the n-type hole barrier region NHB
may be in contact with the p-type body region PB, the gate insulating film GI formed
over the inner wall of the trench T1, and the gate insulating film GI formed over
the inner wall of the trench T2. Also, in the hybrid sub-cell region LCh2, the n-type
hole barrier region NHB may be in contact with the p-type body region PB, the gate
insulating film GI formed over the inner wall of the trench T1, and the gate insulating
film GI formed over the inner wall of the trench T3. As a result, the holes stored
in the n
--type drift region ND are less likely to be discharged into the emitter electrode
EE in each of the hybrid sub-cell regions LCh1 and LCh2. Therefore, an IE effect can
be enhanced.
[0069] In each of the inactive cell regions LCi, the p-type floating region PF as the p-type
semiconductor region is provided under the p-type body region PB to be closer to the
upper surface Sa of the semiconductor substrate SS. That is, in the portion LCi1 of
the inactive cell region LCi, the p-type floating region PF is formed in the portion
of the semiconductor layer SLn which is located opposite to the trench T1 relative
to the trench T2 interposed therebetween. In the portion LCi2 of the inactive cell
region LCi, the p-type floating region PF is formed in the portion of the semiconductor
layer SLn which is located opposite to the trench T1 relative to the trench T3 interposed
therebetween.
[0070] As described above, in the portion LCi1 of the inactive cell region LCi, the end
portion of the p-type floating region PF which is closer to the lower surface Sb is
located closer to the lower surface Sb in the Z-axis direction than the end portion
of the trench T2 which is closer to the lower surface Sb. Also, in the portion LCi2
of the inactive cell region LCi, the end portion of the P-type floating region PF
which is closer to the lower surface Sb is located closer to the lower surface Sb
in the Z-axis direction than the end portion of the trench T3 which is closer to the
lower surface Sb.
[0071] Also, as described above, in the portion LCi1, the p-type floating region PF is preferably
in contact with the gate insulating film GI formed over the inner wall of the trench
T2. Also, in the portion LCi2, the p-type floating region PF is preferably in contact
with the gate insulating film GI formed over the inner wall of the trench T3.
[0072] As shown in FIGS. 4 and 5, in each of the hybrid cell region LCh and the inactive
cell regions LCi, the interlayer insulating film IL made of, e.g., silicon dioxide
or the like is formed over the upper surface Sa of the semiconductor substrate SS.
The interlayer insulating film IL is formed so as to cover the p-type body region
PB in each of the hybrid sub-cell regions LCh1 and LCh2. Note that, between the upper
surface Sa of the semiconductor substrate SS and the interlayer insulating film IL,
an insulating film IF may also be formed.
[0073] In Embodiment 1, in each of the hybrid sub-cell regions LCh1 and LCh2, in the interlayer
insulating film IL and the semiconductor layer SLn, the contact trenches CT are formed
as a plurality of openings each extending through the interlayer insulating film IL
to reach a middle point in the semiconductor layer SLn. In each of the hybrid sub-cell
regions LCh1 and LCh2, the plurality of contact trenches CT are arranged to be spaced
apart from each other in the Y-axis direction in plan view.
[0074] Accordingly, as shown in FIG. 4, in the cross-section along the line A-A in FIG.
3, the contact trenches CT are formed. However, as shown in FIG. 5, in the cross section
along the line B-B in FIG. 3, the contact trenches CT are not formed.
[0075] As shown in FIG. 4, in the cross section along the line A-A in FIG. 3, in each of
the hybrid sub-cell regions LCh1 and LCh2, in the portion of the p-type body region
PB which is exposed at the bottom surface of each of the plurality of contact trenches
CT, the p
+-type body contact region PBC as the p-type semiconductor region is formed. Also,
under the p
+-type body contact region PBC, the p
+-type latch-up preventing region PLP is formed. The p
+-type body contact region PBC and the p
+-type latch-up preventing region PLP form each of the p
+-type semiconductor regions PR.
[0076] That is, in each of the hybrid sub-cell regions LCh1 and LCh2, the p
+-type semiconductor region PR includes the p
+-type body contact region PBC and the p
+-type latch-up preventing region PLP. In each of the hybrid sub-cell regions LCh1
and LCh2, the p-type impurity concentration in the p
+-type body contact region PBC is higher than the p-type impurity concentration in
the p
+-type latch-up preventing region PLP.
[0077] In each of the hybrid sub-cell regions LCh1 and LCh2, the plurality of p
+-type semiconductor regions PR are formed in the portions of the p-type body region
PB which are exposed individually in the plurality of contact trenches CT. Also, as
shown in FIG. 4, in the cross section along the line A-A in FIG. 3, in the hybrid
sub-cell region CLh1, the plurality of p
+-type semiconductor regions PR are formed in the portion of the semiconductor layer
SLn which is located between the trenches T1 and T2. On the other hand, in the hybrid
sub-cell region LCh2, the plurality of p
+-type semiconductor regions PR are formed in the portion of the semiconductor layer
SLn which is located between the trenches T1 and T3.
[0078] In the hybrid sub-cell region CLh1, the p-type impurity concentration in each of
the plurality of p
+-type semiconductor regions PR is higher than the p-type impurity concentration in
the p-type body region PB. In the hybrid sub-cell region CLh2, the p-type impurity
concentration in each of the plurality of p
+-type semiconductor regions PR is higher than the p-type impurity concentration in
the p-type body region PB. In the hybrid sub-cell region LCh1, the plurality of p
+-type semiconductor regions PR are arranged along the Y-axis direction in plan view
to be spaced apart from each other. Also, in the hybrid sub-cell region LCh2, the
plurality of p
+-type semiconductor regions PR are arranged along the Y-axis direction in plan view
to be spaced apart from each other.
[0079] As shown in FIG. 4 which is the cross section along the line A-A in FIG. 3, in each
of the hybrid sub-cell regions LCh1 and LCh2, the plurality of coupling electrodes
CP are formed to be embedded individually in the plurality of contact trenches CT.
[0080] In each of the hybrid sub-cell regions LCh1 and LCh2, the coupling electrodes CP
are in contact with the n
+-type emitter regions NE and the p
+-type semiconductor regions PR. Accordingly, in each of the hybrid sub-cell regions
LCh1 and LCh2, the n
+-type emitter region NE and the plurality of p
+-type semiconductor regions PR are electrically coupled to the emitter electrode EE
via the plurality of coupling electrodes CP.
[0081] In each of the hybrid sub-cell regions LCh1 and LCh2, in each pair of the coupling
electrode CP and the p
+-type semiconductor region PR which are coupled to each other, the coupling electrode
CP is in contact with the p
+-type body contact region PBC included in the p
+-type semiconductor region PR. This can reduce the contact resistance between the
coupling electrode CP and the p
+-type semiconductor region PR.
[0082] As shown in FIGS. 4 and 5, over the interlayer insulating film IL, the emitter electrode
EE made of a metal film containing, e.g., aluminum as a main component is provided.
The emitter electrode EE is coupled to the n
+-type emitter regions NE and the p
+-type body contact regions PBC via the contact trenches CT. In the example shown in
FIG. 4, the coupling electrodes CP and the emitter electrode EE are formed integrally.
[0083] Over the emitter electrode EE, the insulating film FPF as a passivation film made
of, e.g., a polyimide-based organic insulating film or the like is further formed.
[0084] Note that, in the technique disclosed in Patent Document 3 described above, a semiconductor
region equivalent to the p-type floating region PF in the semiconductor device in
Embodiment 1 has not been formed. Also, in the technique disclosed in Patent Document
3 described above, unlike in Embodiment 1, a semiconductor region equivalent to the
p-type body region PB in the semiconductor device in Embodiment 1 is selectively formed
in a longitudinal direction between the trenches.
<Method of Manufacturing Semiconductor Device>
[0085] Next, a method of manufacturing a semiconductor device in Embodiment 1 will be described.
FIGS. 7 to 24 are main-portion cross-sectional views showing the manufacturing process
of the semiconductor device in Embodiment 1. FIGS. 7 to 17, 19, and 21 to 24 are cross-sectional
views along the line A-A in FIG. 3, similarly to FIG. 4. FIGS. 18 and 20 are cross-sectional
views along the line B-B in FIG. 3, similarly to FIG. 5.
[0086] The following will mainly describe the cell formation area AR1 (see FIG. 2). For
the gate-wire-lead-out area AR2 (see FIG. 2), FIG. 2 is referred to as necessary.
The following will also describe the unit cell regions LC each including the hybrid
cell region LCh as the active cell region and the inactive cell regions LCi. As described
above, the hybrid cell region LCh includes the hybrid sub-cell regions LCh1 and LCh2.
[0087] Note that each of the unit cell regions CL includes the positive half portion LCi1
of the inactive cell region LCi which is located on the negative side of the hybrid
cell region LCh in the X-axis direction to be adjacent thereto. Also, the unit cell
region LC includes the negative half portion CLi2 of the inactive cell region CLi
which is located on the positive side of the hybrid cell region CLh in the X-axis
direction to be adjacent thereto.
[0088] First, as shown in FIG. 7, the semiconductor substrate SS made of a silicon single
crystal into which an n-type impurity such as, e.g., phosphorus (P) has been introduced
is provided. The semiconductor substrate SS has the upper surface Sa as the first
main surface and the lower surface Sb as the second main surface opposite to the upper
surface Sa.
[0089] The impurity concentration of the n-type impurity in the semiconductor substrate
SS can be set to, e.g., about 2 x 10
14 cm
-3. At this stage, the semiconductor substrate SS is a thin plate of a semiconductor
having a generally circular two-dimensional shape, which is referred to as a wafer.
The thickness of the semiconductor substrate SS can be set to, e.g., about 450 µm
to 1000 µm.
[0090] Note that, in the semiconductor substrate SS, the semiconductor layer closer to the
upper surface Sa than the semiconductor layer in which the n-type field stop region
Ns (see FIG. 4) is to be formed is assumed to be the semiconductor layer SLn. The
semiconductor layer SLn is an n-type semiconductor layer. It follows therefore that,
when the semiconductor substrate SS is provided, the n-type semiconductor layer SLn
is formed in the semiconductor substrate SS.
[0091] Next, over the entire upper surface Sa of the semiconductor substrate SS, a resist
film R1 for introducing an n-type hole barrier region is formed by coating or the
like and patterned by typical lithography. Using the patterned resist film R1 as a
mask, an n-type impurity is introduced into the upper surface Sa of the semiconductor
substrate SS by, e.g., ion implantation to form the n-type hole barrier regions NHB.
At this time, as a preferred example of conditions for the ion implantation, ion implantation
conditions such that, e.g., an ion species is phosphorus (P), a dose is about 6 x
10
12 cm
-2, and an implantation energy is about 80 KeV can be shown. Then, by ashing or the
like, the unneeded resist film R1 is removed.
[0092] Next, as shown in FIG. 8, over the upper surface Sa of the semiconductor substrate
SS, a resist film R2 for introducing a p-type floating region is formed by coating
or the like and patterned by typical lithography. Using the patterned resist film
R2 as a mask, a p-type impurity is introduced into the upper surface Sa of the semiconductor
substrate SS by, e.g., ion implantation to form the p-type floating region PF. At
this time, as a preferred example of conditions for the ion implantation, ion implantation
conditions such that, e.g., an ion species is boron (B), a dose is about 3.5 x 10
13 cm
-2, and an ion implantation energy is about 75 KeV can be shown. Then, by ashing or
the like, the unneeded resist film R2 is removed. Note that, when the p-type floating
region PF is formed in the cell formation area AR1 (see FIG. 2), the p-type floating
region PFp is formed in, e.g., the gate-wire-lead-out area AR2 (see FIG. 2).
[0093] Next, as shown in FIG. 9, over the upper surface Sa of the semiconductor substrate
SS, a hard mask film HM made of, e.g., silicon dioxide is deposited by, e.g., a CVD
(Chemical Vapor Deposition) method or the like. The hard mask film HM has a thickness
of, e.g., about 450 nm.
[0094] Next, as shown in FIG. 9, over the upper surface Sa of the semiconductor substrate
SS, a resist film R3 for processing a hard mask is formed by coating or the like and
patterned by typical lithography. Using the patterned resist film R3 as a mask, the
hard mask film HM is patterned by, e.g., dry etching.
[0095] Then, as shown in FIG. 10, the unneeded resist film R3 is removed by ashing or the
like.
[0096] Next, as shown in FIG. 11, using the patterned hard mask film HM, the trenches T1,
T2, and T3 are formed by, e.g., anisotropic dry etching. At this time, the trench
T1 is formed to extend from the upper surface Sa of the semiconductor substrate SS
in the Y-axis direction in plan view and reach a middle point in the semiconductor
layer SLn. Also, the trenches T2 and T3 are formed to extend in the Y-axis direction
in plan view from the upper surface Sa of the semiconductor substrate SS, reach middle
points in the semiconductor layer SLn, and be located on both sides of the trench
T1 interposed therebetween. As a gas for the anisotropic dry etching, e.g., a Cl
2/O
2-based gas can be shown as a preferred example.
[0097] Then, as shown in FIG. 12, by wet etching using, e.g., a hydrofluoric-acid-based
etching solution or the like, the unneeded hard mask HM is removed.
[0098] Next, as shown in FIG. 13, extension diffusion (e.g., at 1200 °C for about 30 minutes)
is performed on the p-type floating regions PF and the n-type hole barrier regions
NHB. At this time, the extension diffusion is performed such that the end portion
of the p-type floating region PF which is closer to the lower surface Sb is located
closer to the lower surface Sb in the Z-axis direction than the respective end portions
of the trenches T1, T2, and T3 which are closer to the lower surface Sb.
[0099] Thus, in the portion of the semiconductor layer SLn which is located opposite to
the trench T1 relative to the trench T2 interposed therebetween, the p-type floating
region PF is formed and, in the portion of the semiconductor layer SLn which is located
opposite to the trench T1 relative to the trench T3 interposed therebetween, the p-type
floating regions PF are formed. Preferably, the p-type floating region PF formed opposite
to the trench T1 relative to the trench T2 interposed therebetween is in contact with
the gate insulating film GI formed over the inner wall of the trench T2, and the p-type
floating region PF formed opposite to the trench T1 relative to the trench T3 interposed
therebetween is in contact with the gate insulating film GI formed over the inner
wall of the trench T3.
[0100] Additionally, the end portion of the p-type floating region PF formed opposite to
the trench T1 relative to the trench T2 interposed therebetween which is closer to
the lower surface Sb is located closer to the lower surface Sb in the Z-axis direction
than the end portion of the trench T2 which is closer to the lower surface Sb. Also,
the end portion of the p-type floating region PF formed opposite to the trench T1
relative to the trench T3 interposed therebetween which is closer to the lower surface
Sb is located closer to the lower surface Sb in the Z-axis direction than the end
portion of the trench T3 which is closer to the lower surface Sb.
[0101] In addition, in the portion of the semiconductor layer SLn which is located between
the trenches T1 and T2 and the portion of the semiconductor layer SLn which is located
between the trenches T1 and T3, the n-type hole barrier regions NHB are formed. Preferably,
the n-type hole barrier region NHB formed between trenches T1 and T2 is in contact
with the gate insulating film GI formed over the inner wall of the trench T1 and with
the gate insulating film GI formed over the inner wall of the trench T2. Preferably,
the n-type hole barrier region NHB formed between the trenches T1 and T3 is in contact
with the gate insulating film GI formed over the inner wall of the trench T1 and with
the gate insulating film GI formed over the inner wall of the trench T3.
[0102] During the extension diffusion, the region of the n-type semiconductor substrate
SS where the p-type floating regions PF and the n-type hole barrier regions NHB are
not formed serves as the n
--type drift region ND. In other words, the region of the n-type semiconductor layer
SLn where the p-type floating regions PF and the n-type hole barrier regions NHB are
not formed serves as the n-type drift region ND. Note that, in the process step shown
in FIG. 13, the n
--type drift region ND is formed to extend from within the semiconductor layer SLn
to the lower surface Sb of the semiconductor substrate SS.
[0103] Between the trenches T1 and T2, the n-type impurity concentration in the n-type hole
barrier region NHB is higher than the n-type impurity concentration in the portion
of the semiconductor layer SLn which is located closer to the lower surface Sb than
the n-type hole barrier region NHB, i.e., in the n
--type drift region ND and lower than the n-type impurity concentration in each of
the n
+-type emitter regions NE. What applies to the n-type impurity concentration in the
n-type hole barrier region NHB between the trenches T1 and T2 similarly applies to
the n-type impurity concentration in the n-type hole barrier region NHB between the
trenches T1 and T3.
[0104] Next, as shown in FIG. 13, by, e.g., a thermal oxidation method or the like, the
gate insulating film GI made of, e.g., silicon dioxide is formed over the upper surface
Sa of the semiconductor substrate SS and the respective inner walls of the trenches
T1, T2, and T3. The thickness of the gate insulating film GI is, e.g., about 0.12
µm.
[0105] Next, as shown in FIG. 14, over the upper surface Sa of the semiconductor substrate
SS and in each of the trenches T1, T2, and T3, a conductive film CG made of polycrystalline
silicon doped with phosphorus (P) (Doped Poly-Silicon) is deposited by, e.g., a CVD
method or the like. The thickness of the conductive film CF is. e.g., about 0.6 µm.
[0106] Next, as shown in FIG. 15, by, e.g., dry etching or the like, the conductive film
CF is etched back. Thus, the trench gate electrode TG1 made of the conductive film
CF embedded in the trench T1 via the gate insulating film GI is formed. Also, the
trench gate electrode GT2 made of the conductive film CF embedded in the trench T2
via the gate insulating film GI is formed. Also, the trench gate electrode GT3 made
of the conductive film CF embedded in the trench T3 via the gate insulating film GI
is formed.
[0107] In other words, over the gate insulating film GI, the trench gate electrode TG1 is
formed so as to be embedded in the trench T1 and, over the gate insulating film GI,
the trench gate electrode TG2 is formed so as to be embedded in the trench T2 and,
over the gate insulating film GI, the trench gate electrode TG3 is formed so as to
be embedded in the trench T3. As a preferred example of a gas for the etching, e.g.,
a SF
6 gas or the like can be shown.
[0108] Next, as shown in FIG. 16, the gate insulating film GI except for the portions thereof
located in the trenches T1, T2, and T3 is removed by dry etching or the like.
[0109] Next, as shown in FIG. 17, over the upper surface Sa of the semiconductor substrate
SS, the insulating film IF made of a relatively thin silicon dioxide film (which is
as thin as, e.g., the gate insulating film GI) for subsequent ion implantation is
formed by, e.g., thermal oxidation or CVD. Next, over the upper surface Sa of the
semiconductor substrate SS, a resist film (the depiction thereof is omitted) for introducing
a p-type body region is formed by typical lithography. Using the resist film for introducing
the p-type body region as a mask, a p-type impurity is introduced into the entire
surface of the cell formation area AR1 and other regions into which the p-type impurity
needs to be introduced to form the p-type body region PB.
[0110] Specifically, in the portion of the semiconductor layer SLn which is located between
the trenches T1 and T2, the p-type body region PB is formed to be in contact with
the gate insulating film GI formed over the inner wall of the trench T1 and with the
gate insulating film GI formed over the inner wall of the trench T2. Also, in the
portion of the semiconductor layer SLn which is located between the trenches T1 and
T3, the p-type body region PB is formed to be in contact with the gate insulating
film GI formed over the inner wall of the trench T1 and with the gate insulating film
GI formed over the inner wall of the trench T3.
[0111] At this time, as a preferred example of conditions for the ion implantation, ion
implantation conditions such that, e.g., an ion species is boron (B), a dose is about
3 x 10
13 cm
-2, and an implantation energy is about 75 KeV can be shown. Then, by ashing or the
like, the unneeded resist film for introducing the p-type body region is removed.
[0112] Then, over the upper surface Sa of the semiconductor substrate SS, a resist film
(the depiction thereof is omitted) for introducing n
+-type emitter regions is formed by typical lithography. Using the resist film for
introducing the n
+-type emitter regions as a mask, an n-type impurity is introduced into the upper-layer
portion of the p-type body region PB of the hybrid cell region LCh by, e.g., ion implantation
to form the n
+-type emitter regions NE.
[0113] Specifically, in the portion of the semiconductor layer SLn which is located between
the trenches T1 and T2, the n
+-type emitter region NE is formed to be in contact with the gate insulating film GI
formed over the inner wall of the trench T1 and with the p-type body region PB. Also,
in the portion of the semiconductor layer SLn which is located between the trenches
T1 and T3, the n
+-type emitter region NE is formed to be in contact with the gate insulating film GI
formed over the inner wall of the trench T1 and with the p-type body region PB.
[0114] At this time, as a preferred example of conditions for the ion implantation, ion
implantation conditions such that, e.g., an ion species is arsenic (As), a dose is
about 5 x 10
15 cm
-2, and an implantation energy is about 80 KeV can be shown. Then, by ashing or the
like, the unneeded resist film for introducing the n
+-type emitter regions is removed.
[0115] Here, the cross section shown in FIG. 17 is equivalent to the cross section along
the line A-A in FIG. 3, i.e., the cross section shown in FIG. 4. On the other hand,
in the cross section along the line B-B in FIG. 3, i.e., in a cross section equivalent
to the cross section shown in FIG. 5, the n
+-type emitter regions NE are not formed so that a state as shown in FIG. 18 is reached.
[0116] Next, as shown in FIG. 19, over the upper surface Sa of the semiconductor substrate
SS, the interlayer insulating film IL made of, e.g., a PSG (Phosphosilicate Glass)
film is formed by, e.g., a CVD method or the like. The interlayer insulating film
IL is formed so as to cover the p-type body region PB via the insulating film IF.
The interlayer insulating film IL has a thickness of, e.g., about 0.6 µm. As preferred
examples of the material of the interlayer insulating film IL, not only the PSG film,
but also a BPSG (Borophosphosilicate Glass film), an NSG (Non-doped Silicate Glass)
film, a SOG (Spin-On-Glass) film, a composite film thereof, or the like can be shown.
[0117] Here, the cross section shown in FIG. 19 is equivalent to the cross section along
the line A-A in FIG. 3, i.e., the cross section shown in FIG. 4. On the other hand,
in the cross section along the line B-B in FIG. 3, i.e., in the cross section equivalent
to the cross section shown in FIG. 5, the n
+-type emitter regions NE are not formed so that a state as shown in FIG. 20 is reached.
[0118] Next, as shown in FIG. 21, over the interlayer insulating film IL, a resist film
(the depiction thereof is omitted) for forming contact trenches is formed by typical
lithography. Subsequently, the contact trenches CT are formed by, e.g., anisotropic
dry etching or the like. As a preferred example of a gas used for the anisotropic
dry etching, a gas mixture including, e.g., an Ar gas, a CHF
3 gas, and a CF
4 gas or the like can be shown. Then, the unneeded resist film for forming the contact
trenches is removed by ashing or the like.
[0119] Next, as shown in FIG. 21, the contact trenches CT are extended into the semiconductor
substrate SS by, e.g., anisotropic dry etching. As a preferred example of the gas
for the anisotropic dry etching, e.g., a Cl
2/O
2 gas can be shown.
[0120] Here, the cross section shown in FIG. 21 is equivalent to a cross section along the
line A-A in FIG. 3, i.e., the cross section shown in FIG. 4. On the other hand, in
a cross section along the line B-B in FIG. 3, i.e., a cross section equivalent to
the cross section shown in FIG. 5, the contact trenches CT are not formed. As a consequence,
the cross section along the line B-B in FIG. 3 remains unchanged from the cross section
shown in FIG. 20.
[0121] Accordingly, by performing the process step shown in FIG. 21, the contact trenches
CT are formed as a plurality of openings each extending through the interlayer insulating
film IL in the hybrid sub-cell region LCh1 and reaching a middle point in the p-type
body region PB. In the hybrid sub-cell region LCh1, the plurality of contact trenches
CT are arranged along the Y-axis direction in plan view to be spaced apart from each
other.
[0122] Also, by performing the process step shown in FIG. 21, in the hybrid sub-cell region
LCh2, the contact trenches CT are formed as a plurality of openings each extending
through the interlayer insulating film IL and reaching a middle point in the p-type
body region PB. In the hybrid sub-cell region LCh2, the plurality of contact trenches
CT are arranged along the Y-axis direction in plan view to be spaced apart from each
other.
[0123] Next, as shown in FIG. 22, a p-type impurity is ion-implanted through, e.g., the
contact trenches CT to form the p
+-type body contact regions PBC. Here, as a preferred example of conditions for the
ion implantation, ion implantation conditions such that, e.g., an ion species is boron
(B), a dose is about 5 x 10
15 cm
-2, and an implantation energy is about 80 KeV can be shown.
[0124] Likewise, a p-type impurity is ion-implanted through, e.g., the contact trenches
CT to form the p
+-type latch-up preventing regions PLP. Here, as a preferred example of conditions
for the ion implantation, ion implantation conditions such that, e.g., an ion species
is boron (B), a dose is about 5 x 10
15 cm
-2, and an implantation energy is about 80 KeV can be shown. The p-type impurity concentration
in each of the p
+-type body contact regions PBC is higher than the p-type impurity concentration in
each of the p
+-type latch-up preventing regions PLP. The p
+-type body contact region PBC and the p
+-type latch-up preventing region PLP form the p
+-type semiconductor region PR.
[0125] The cross section shown in FIG. 22 is equivalent to the cross section along the line
A-A in FIG. 3, i.e., the cross section shown in FIG. 4. On the other hand, in a cross
section along the line B-B in FIG. 3, i.e., a cross section equivalent to the cross
section shown in FIG. 5, the p
+-type semiconductor regions PR each including the p
+-type body contact region PBC and the p
+-type latch-up preventing region PLP are not formed. As a consequence, the cross section
along the line B-B in FIG. 3 remains unchanged from the cross section shown in FIG.
20.
[0126] Accordingly, by performing the process step shown in FIG. 22, in the hybrid sub-cell
region LCh1, in each of the portions of the p-type body region PB which are exposed
in the individual contact trenches CT, the plurality of p
+-type semiconductor regions PR are formed. In the hybrid sub-cell region LCh1, the
plurality of p
+-type semiconductor regions PR are arranged along the Y-axis direction in plan view
to be spaced apart from each other.
[0127] Also, by performing the process step shown in FIG. 22, in the hybrid sub-cell region
LCH2, in the portions of the p-type body region PB which are exposed in the individual
contact trenches CT, the plurality of p
+-type semiconductor regions PR are formed. In the hybrid sub-cell region LCh2, the
plurality of p
+-type semiconductor regions PR are arranged along the Y-axis direction in plan view
to be spaced apart from each other.
[0128] That is, by performing the process step shown in FIG. 22, in the portion of the semiconductor
layer SLn which is located between the trenches T1 and T2, the plurality of p
+-type semiconductor regions PR are each formed to be in contact with the p-type body
region PB. Also, in the portion of the semiconductor layer SLn which is located between
the trenches T1 and T3, the plurality of p
+-type semiconductor regions PR are each formed to be in contact with the p-type body
region PB. In each of the hybrid sub-cell regions LCh1 and LCh2, the p-type impurity
concentration in each of the plurality of p
+-type semiconductor regions PR is higher than the p-type impurity concentration in
the p-type body region PB.
[0129] In the manufacturing process of the semiconductor device in Embodiment 1, the plurality
of contact trenches CT are formed to be arranged along the Y-axis direction in plan
view and spaced apart from each other. Then, using the interlayer insulating film
IL formed with the plurality of contact trenches CT as a mask, the plurality of p
+-type semiconductor regions PR can be formed to be arranged along the Y-axis direction
in plan view and spaced apart from each other. Accordingly, in the manufacturing process
of the semiconductor device in Embodiment 1, an additional mask for forming the plurality
of p
+-type semiconductor regions PR need not be provided and additional lithography for
forming the plurality of p
+-type semiconductor regions PR need not be performed.
[0130] Next, as shown in FIG. 23, the emitter electrode EE is formed. Specifically, the
formation of the emitter electrode EE is performed in accordance with, e.g., the following
procedure. First, over the upper surface Sa of the semiconductor substrate SS, a TiW
film is formed as a barrier metal film by, e.g., sputtering. The TiW film has a thickness
of, e.g., about 0.2 µm. The major part of titanium in the TiW film moves to the silicon
interface as a result of subsequent heat treatment to form a silicide and contribute
to an improvement in contact characteristic. However, such a process is intricate
and is therefore not shown in the drawing.
[0131] Next, silicide anneal is performed for about 10 minutes in a nitrogen atmosphere
at, e.g., about 600 °C. Then, over the entire upper surface of the barrier metal film,
an aluminum-based metal film (which contains several percent of added silicon and
the remaining part of which is aluminum) is formed by, e.g., sputtering so as to be
embedded in the contact trenches CT. The aluminum-based metal film has a thickness
of, e.g., about 5 µm.
[0132] Next, by typical lithography, a resist film (the depiction thereof is omitted) for
forming an emitter electrode is formed. Subsequently, the emitter electrode EE including
the aluminum-based metal film and the barrier metal film is patterned by, e.g., dry
etching. As a preferred example of a gas for the dry etching, e.g., a Cl
2/BCI
3 gas or the like can be shown. Then, the unneeded resist film for forming the emitter
electrode is removed by ashing or the like.
[0133] Here, the cross section shown in FIG. 23 is equivalent to the cross section along
the line A-A in FIG. 3, i.e., the cross section shown in FIG. 4. On the other hand,
in the cross section along the line B-B in FIG. 3, the contact trenches CT are not
formed so that a cross section as shown in FIG. 5 is obtained.
[0134] By performing the process step shown in FIG. 23, in the hybrid sub-cell region LCh1,
the plurality of coupling electrodes CP embedded individually in the plurality of
contact trenches CT and the emitter electrode EE formed over the interlayer insulating
film IL are formed. In the hybrid sub-cell region LCh1, the plurality of coupling
electrodes CP are arranged along the Y-axis direction in plan view to be spaced apart
from each other. Also, by performing the process step shown in FIG. 23, in the hybrid
sub-cell region LCh2, the plurality of coupling electrodes CP embedded individually
in the plurality of contact trenches CT and the emitter electrode EE formed over the
interlayer insulating film IL are formed. In the hybrid sub-cell region LCh2, the
plurality of coupling electrodes CP are arranged along the Y-axis direction in plan
view to be spaced apart from each other.
[0135] The emitter electrode EE is electrically coupled to the n
+-type emitter regions NE and the plurality of p
+-type semiconductor regions PR which are formed in each of the hybrid sub-cell regions
LCh1 and LCh2 via the plurality of coupling electrodes CP formed in the hybrid sub-cell
region. Note that, when the emitter electrode EE is formed, the gate electrode GE
(see FIG. 1) electrically coupled to the trench gate electrode TG1 may also be formed.
[0136] Note that, when the emitter electrode EE is formed in the cell formation area AR1
(see FIG. 2), the gate wire GL and the gate electrode GE (see FIG. 1) can be formed
in the gate-wire-pull-out area AR2 (see FIG. 2).
[0137] Next, as shown in FIG. 23, over the emitter electrode EE, the insulating film FPF
is formed as a passivation film made of an organic film containing, e.g., polyimide
as a main component or the like. The insulating film FPF has a thickness of, e.g.,
about 2.5 µm.
[0138] Next, by typical lithography, a resist film (the depiction thereof is omitted) for
forming openings is formed. Next, the insulating film FPF is patterned by, e.g., dry
etching to be formed with the opening OP (see FIG. 1) extending through the insulating
film FPF to reach the emitter electrode EE and form the emitter pad EP (see FIG. 1)
made of the portion of the emitter electrode EE which is exposed in the opening OP1.
Then, by ashing or the like, the unneeded resist film for forming the openings is
removed.
[0139] Note that, when the insulating film FPF is formed over the emitter electrode EE in
the cell formation area AR1 (see FIG. 1), the insulating film FPF is formed over the
gate electrode GE (see FIG. 1) in the gate-wire-lead-out area AR2 (see FIG. 1). Also,
when the opening OP1 is formed in the cell formation area AR1 (see FIG. 1), the opening
OP2 (see FIG. 1) is formed in the gate-wire-lead-out area AR2 (see FIG. 1) to extend
through the insulating film FPF and reach the gate electrode GE, and the gate pad
GP made of the portion of the gate electrode GE which is exposed in the opening OP2
is formed.
[0140] Next, as shown in FIG. 24, back grinding treatment is performed on the lower surface
Sb of the semiconductor substrate SS to reduce a thickness of, e.g., about 800 µm
to, e.g., about 30 to 200 µm as necessary. When a breakdown voltage is, e.g., about
600 V, a final thickness is about 70 µm. Thus, in the portion of the thinned semiconductor
substrate SS which is located closer to the lower surface Sb than the semiconductor
layer SLn, the semiconductor layer SLp is formed. In addition, chemical etching or
the like for removing damage to the lower surface Sb or the like is also performed
as necessary.
[0141] In the thinned semiconductor substrate SS, a semiconductor layer which is closer
to the lower surface Sb than the semiconductor layer where the n-type field stop region
Ns (see FIG. 4) is to be formed and in which the p
+-type collector region CL (see FIG. 4) is to be formed is assumed to be the semiconductor
layer SLp.
[0142] Next, as shown in FIG. 4, into the lower surface Sb of the semiconductor substrate
SS, an n-type impurity is introduced by, e.g., ion implantation to form the n-type
field stop region Ns. Here, as a preferred example of conditions for the ion implantation,
ion implantation conditions such that, e.g., an ion species is phosphorus (P), a dose
is about 7 x 10
12 cm
-2, and an implantation energy is about 350 KeV can be shown. Then, as necessary, laser
anneal or the like is performed on the lower surface Sb of the semiconductor substrate
SS so as to activate the impurity.
[0143] Next, into the lower surface Sb of the semiconductor substrate SS, a p-type impurity
is introduced by, e.g., ion implantation to form the p
+-type collector region CL. Here, as a preferred example of conditions for the ion
implantation, ion implantation conditions such that, e.g., an ion species is boron
(B), a dose is about 1 x 10
13 cm
-2, and an implantation energy is about 40 KeV can be shown. Then, as necessary, laser
anneal or the like is performed on the lower surface Sb of the semiconductor substrate
SS so as to activate the impurity.
[0144] That is, in the step of forming the p
+-type collector region CL, the p-type semiconductor layer SLp is formed in the portion
of the semiconductor substrate SS which is located closer to the lower surface Sb
than the semiconductor layer SLn. The p
+-type collector region CL is formed of the p-type semiconductor layer SLp.
[0145] Next, by, e.g., sputtering, over the lower surface Sb of the semiconductor substrate
SS, the collector electrode CE electrically coupled to the semiconductor layer SLp,
i.e., the p
+-type collector region CL is formed. Then, by dicing or the like, the semiconductor
substrate SS is divided by dicing or the like into chip regions, each of which is
encapsulated in a package as necessary to complete the semiconductor device in Embodiment
1.
<Semiconductor Device in Comparative Example 1>
[0146] Next, a description will be given of a semiconductor device in Comparative Example
1. The semiconductor device in Comparative Example 1 includes an IGBT having a GG-type
(gate-gate-type) active cell region. Note that the possession of the GG-type active
cell region by the IGBT means that each of two trench gate electrodes located to be
spaced apart from each other in the active cell region is electrically coupled to
the gate electrode.
[0147] FIG. 25 is a main-portion plan view of the semiconductor device in Comparative Example
1.
[0148] In the semiconductor device in Comparative Example 1, each of the unit cell regions
LC includes a GG-type active cell region LCa and the two inactive cell regions LCi.
That is, in the semiconductor device in Comparative Example 1, the unit cell region
LC includes the GG-type active cell region LCa instead of the hybrid cell region LCh
as the EGE-type active cell region in the semiconductor device in Embodiment 1.
[0149] The two unit cell regions LC adjacent to each other in an X-axis direction share
the one inactive cell region LCi. Accordingly, each of the unit cell regions LC has
the positive half portion LCi1 of the inactive cell region LCi which is located on
the negative side of the active cell region LCa in the X-axis direction to be adjacent
thereto. The unit cell region LC also has the negative half portion LCi2 of the inactive
cell region LCi which is located on the positive side of the active cell region LCa
in the X-axis direction to be adjacent thereto.
[0150] The active cell region LCa is the same as the hybrid sub-cell region LCh1 in the
semiconductor device in Embodiment 1 except that the n
+-type emitter regions NE are located on both sides of the coupling electrode CP interposed
therebetween. The active cell region LCa includes the trench gate electrodes TG1 and
TG2. The trench gate electrode TG1 is interposed between the active cell region LCa
and the portion LCi2 of the inactive cell region LCi. The trench gate electrode TG2
is located between the active cell region LCa and the portion LCi1 of the inactive
cell region LCi. Note that, in Comparative Example 1, not only the trench gate electrode
TG1, but also the trench gate electrode TG2 is electrically coupled to the gate electrode
GE (see FIG. 1).
[0151] The n
+-type emitter regions NE are formed in the portion of the semiconductor layer SLn
which is located between the trenches T1 and T2 and located on both sides of the coupling
electrode CP interposed therebetween. That is, as the n
+-type emitter regions NE, not only a region in contact with the p-type body region
PB and with the gate insulating film IG formed over the inner wall of the trench T1,
but also a region in contact with the p-type body region PB and with the gate insulating
film GI formed over the inner wall of the trench T2 is formed.
<Semiconductor Device in Comparative Example 2>
[0152] Next, a description will be given of a semiconductor device in Comparative Example
2. The semiconductor device in Comparative Example 2 includes an IGBT having an EGE-type
active cell region.
[0153] FIGS. 26 and 27 are main-portion plan views of the semiconductor device in Comparative
Example 2. FIG. 28 is a main-portion cross-sectional view of the semiconductor device
in Comparative Example 2. FIG. 28 is a cross-sectional view along the line C-C in
FIG. 27. Note that a cross-sectional view along the line A-A in FIG. 27 is the same
as the cross-sectional view shown in FIG. 4. Also, a cross-sectional view along the
line B-B in FIG. 27 is the same as the cross-sectional view shown in FIG. 4 except
that the n
+-type emitter regions NE are not provided.
[0154] In the semiconductor device in Comparative Example 2, in the same manner as in the
semiconductor device in Embodiment 1, each of the unit cell regions LC includes the
hybrid cell region LCh as an active cell region and the two inactive cell regions
LCi. Also, in the semiconductor device in Comparative Example 2, in the same manner
as in the semiconductor device in Embodiment 1, the plurality of n
+-type emitter regions NE are formed in each of the hybrid sub-cell regions LCh1 and
LCh2.
[0155] On the other hand, in Comparative Example 2, unlike in Embodiment 1, in the hybrid
sub-cell region LCh1, the p
+-type semiconductor regions PR are formed continuously along the Y-axis direction.
The plurality of p
+-type semiconductor regions PR are arranged along the Y-axis direction in plan view
to be spaced apart from each other. Also, in the hybrid sub-cell region LCh1, the
contact trenches CT as openings are formed continuously along the Y-axis direction
in the p-type body region PB. The contact trenches CT reach the p
+-type body contact region PBC located in the hybrid sub-cell region LCh1.
[0156] Also, in Comparative Example 2, unlike in Embodiment 1, in the hybrid sub-cell region
LCh2, the p
+-type semiconductor regions PR are formed continuously along the Y-axis direction.
The plurality of p
+-type semiconductor regions PR are arranged along the Y-axis direction in plan view
to be spaced apart from each other. Also, in the hybrid sub-cell region LCh2, the
contact trenches CT as the openings are formed continuously along the Y-axis direction
in the p-type body region PB. The contact trenches CT reach the p
+-type body contact region PBC located in the hybrid sub-cell region LCh2.
<About Advantage of Semiconductor Device in Comparative Example 2>
[0157] Next, a description will be given of the advantage of the semiconductor device in
Comparative Example 2 over the semiconductor device in Comparative Example 1.
[0158] FIG. 29 is a cross-sectional view showing displacement current paths resulting from
the charging up of a floating region due to the storage of carriers (holes) when the
semiconductor device in Comparative Example 1 is turned ON in overlapping relation.
FIG. 30 is an equivalent circuit diagram showing the displacement current paths resulting
from the charging up of the floating region due to the storage of carriers (holes)
when the semiconductor device in Comparative Example 1 is turned ON. FIG. 31 is a
cross-sectional view showing displacement current paths resulting from the charging
up of a floating region due to the storage of carriers (holes) when the semiconductor
device in Comparative Example 2 is turned ON in overlapping relation. FIG. 32 is an
equivalent circuit diagram showing the displacement current paths resulting from the
charging up of the floating region due to the storage of carriers (holes) when the
semiconductor device in Comparative Example 2 is turned ON.
[0159] Note that displacement current paths resulting from a rise in collector voltage at
a turn-OFF time are the same displacement current paths as the displacement current
paths at the turn-ON time shown in FIGS. 29 to 32, except that the directions of the
arrows showing the displacement currents are opposite.
[0160] As shown in FIGS. 29 and 30, in the semiconductor device in Comparative Example 1
including the IGBT having the GG-type active cell region, the p-type floating region
PF is adjacent, via the gate insulating film GI, to each of the trench gate electrodes
TG1 and TG2 coupled to the gate electrode GE. The semiconductor device in Comparative
Example 1 can be represented by an equivalent circuit using an IGBT 1 including the
collector electrode CE, the emitter electrode EE, the gate electrode GE, capacitances
Cgd, Cgs, Cfpc, and Cgfp, and a resistance Rg coupled to the gate electrode GE. In
the semiconductor device in Comparative Example 1, a displacement current CR100 generated
in the unit cell region LC flows into the gate electrode GE. Accordingly, the displacement
current CR100 exerts large influence on the potential of the gate electrode GE, i.e.,
gate potential.
[0161] On the other hand, as shown in FIGS. 31 and 32, in the semiconductor device in Comparative
Example 2 including the EGE-type active cell region, the p-type floating region PF
and the trench gate electrode TG1 coupled to the gate electrode GE are cut off by
each of the trench gate electrodes TG2 and TG3 coupled to the emitter electrode EE
and are not adjacent to each other. The semiconductor device in Comparative Example
2 can be represented by an equivalent circuit using the IGBT 1 including the collector
electrode CE, the emitter electrode EE, the gate electrode GE, the capacitances Cgd,
Cgs, Cfpc, Ced, and Cefp, and the resistance Rg coupled to the gate electrode GE.
A displacement current CR1 generated in the unit cell region LC flows into the emitter
electrode EE, but does not flow into the gate electrode GE. Accordingly, the displacement
current CR1 exerts small influence on the potential of the gate electrode GE, i.e.,
gate potential.
[0162] In Comparative Example 1, the displacement current CR100 generated in the active
cell region LCa may flow into the gate electrode GE via a feedback capacitance made
of the capacitance Cgd shown in FIGS. 29 and 30. On the other hand, in Comparative
Example 2, the displacement current CR2 generated in the hybrid cell region LCh may
flow into the gate electrode GE via a feedback capacitance made of the capacitance
Cgd shown in FIGS. 31 and 32. Accordingly, to reduce the influence exerted by each
of the displacement currents on the potential of the gate electrode GE, the capacitance
Cgd as the feedback capacitance needs to be minimized.
[0163] On the other hand, the semiconductor device in Comparative Example 2 having the EGE-type
active cell region has the advantage of being able to reduce the capacitance Cgd as
the feedback capacitance over the semiconductor device in Comparative Example 1 having
the GG-type active cell region. Accordingly, a circuit formed of the semiconductor
device in Comparative Example 2, such as an inverter circuit, has an advantage in
that fluctuation is less likely to occur in the output of the circuit than in a circuit
formed of the semiconductor device in Comparative Example 1, such as an inverter circuit.
[0164] Next, as shown in FIG. 32, a description will be given of the operation of a p-channel
parasitic MOSFET (Metal Oxide Semiconductor Field Effect Transistor) 2 formed in the
IGBT 1. FIG. 33 is a cross-sectional view showing a p-channel parasitic MOSFET in
the semiconductor device in Comparative Example 2.
[0165] The following will describe an example in which the parasitic MOSFET is formed in
the IGBT 1. However, it may also be possible that, in the IGBT 1, a parasitic MISFET
made of any of various MISFETs (Metal Insulator Semiconductor Field Effect Transistors)
other than a MOSFET is formed.
[0166] The following will consider an operation when the semiconductor device in Comparative
Example 2 is turned OFF by L-load switching. When the semiconductor device in Comparative
Example 2 is turned OFF by the L-load switching, a voltage VCE as a collector-emitter
voltage rises upon the turning OFF. At this time, the conductivity type of the channel
region of a p-channel parasitic MOSFET 2 is inverted to a p-type. Consequently, holes
as the carriers stored in the p-type floating region PF and the n
- -type drift region ND are discharged via the p-channel parasitic MOSFET 2. By the
foregoing operation, the stored holes are promptly discharged so that the semiconductor
device in Comparative Example 2 has the advantage of a higher switching speed over
the semiconductor device in Comparative Example 1.
[0167] Next, a description will be given of a process in which the p-channel parasitic MOSFET
2 is brought into an ON state when the semiconductor device in Comparative Example
2 is turned OFF and the holes as the stored carriers are discharged. By way of example,
the following will describe the result of calculation performed using TCAD (Technology
Computer-Aided Design).
[0168] FIG. 34 is a circuit diagram showing an equivalent circuit in an L-load switching
test. FIG. 35 is a view schematically showing a switching waveform in the L-load switching
test. FIGS. 36 and 37 are graphs showing switching waveforms when the semiconductor
device in Comparative Example 2 is turned OFF. FIG. 38 is a cross-sectional view showing
a hole density distribution when the semiconductor device in Comparative Example 2
is turned OFF.
[0169] Note that the results shown in FIGS. 36, 37, and 38 are obtained by calculation performed
using the TCAD. The calculation using the TCAD was performed using the following numerical
values, though the display of specific numerical values is omitted in the graphs of
FIGS. 36, 37, and 38. That is, the impurity concentration in the n
--type drift region, i.e., the semiconductor layer SLn was set to 6.1 x 10
13 cm
-3. The thickness of the semiconductor layer SLn was set to 70 µm. The temperature was
set to a room temperature. A power supply potential VCC (see FIG. 34) was set to 400
V. A current IC as a collector current was set to 50 A. An inductance L (see FIG.
34) was set to 200 µH. In addition, a voltage VGE as a gate-emitter voltage was varied
between -15 V and +15 V.
[0170] FIG. 36 shows the time dependences of the voltage VGE as the gate-emitter voltage,
the voltage VCE as the collector-emitter voltage, and the current IC as the collector
current. FIG. 37 shows the time dependences of a hole current density Jp, a hole density
Np, and a potential Vch as the potential of the channel region of the p-channel parasitic
MOSFET. The abscissa axis in each of FIGS. 36 and 37 shows the same time range.
[0171] Note that FIGS. 36 and 37 show the time dependences in the two cases where the impurity
concentration in each of the n-type hole barrier regions NHB is low and where the
impurity concentration in each of the n-type hole barrier regions NHB is high. Since
the influence of the impurity concentration in the n-type hole barrier region NHB
will be described later, a description is given here of the case where the impurity
concentration in the n-type hole barrier region NHB is low.
[0172] In an equivalent circuit at the time of L-load switching, a driver 3, the resistance
Rg, the IGBT 1, a FRD (Fast Recovery Diode) 4, the inductance L, a capacitance C,
and the power supply potential VCC are coupled to each other, as shown in FIG. 34.
[0173] As shown in FIG. 35, when the voltage VGE as a switching waveform including first
and second two pulses is applied to the semiconductor device including the IGBT, the
switching characteristic of the semiconductor device at a turn-OFF time is measured
as the switching characteristic at a turn-ON time when the first pulse is applied.
[0174] As shown in FIG. 36, at the turn-OFF time, the voltage VCE rises as the voltage VGE
drops and the current IC decreases. Also, as shown in FIG. 37, as the voltage VGE
drops, the voltage VCE rises, and the current IC decreases, the potential Vch rises,
the hole current density Jp increases, and the hole density Np increases. From the
foregoing, it will be understood that, when the IGBT included in the semiconductor
device is turned OFF, the potential of the channel region of the p-channel parasitic
MOSFET rises to bring the parasitic MOSFET into the ON state and holes as carriers
are discharged.
[0175] Also, in the hole density distribution shown in FIG. 38, the hole densities are higher
in the respective portions of the p-type floating regions PF, the n-type hole barrier
regions NHB, and the p-type body regions PB which are closer to the trenches T2 and
T3 and lower in the respective portions of the p-type floating regions PF, the n-type
hole barrier regions NHB, and the p-type body regions PB which are further away from
the trenches T2 and T3, except in the p
+-type semiconductor regions PR where the hole densities are originally high.
[0176] Consequently, as shown in FIG. 38, a hole current flows through each of current paths
PT1 each extending from the n
--type drift region ND through the p-type floating region PF and also through the respective
portions of the p-type floating region PF, the n-type hole barrier region NHB, and
the p-type body region PB which are closer to the trenches T2 and T3. Also, as shown
in FIG. 38, a hole current flows through each of current paths PT2 each extending
from the n
--type drift region ND through the n-type hole barrier region NHB and also through
the respective portions of the n-type hole barrier region NHB and the p-type body
region PB which are closer to the trenches T2 and T3.
<About Problems of Semiconductor Device in Comparative Example 2>
[0177] The semiconductor device including the IGBT having the EGE-type active cell region
(semiconductor device in Comparative Example 2) also has problems which do not affect
the semiconductor device including the IGBT having the GG-type active cell region
(semiconductor device in Comparative Example 1). The following will describe the problems
of the semiconductor device in Comparative Example 2 which do not affect the semiconductor
device in Comparative Example 1.
[0178] First, a description will be given of a rise in ON voltage.
[0179] FIGS. 39 to 41 are graphs showing the collector-emitter voltage dependences of collector
currents in the semiconductor devices in Comparative Examples 1 and 2 in the ON state.
The abscissa axis in each of FIGS. 39 to 41 shows the voltage VCE as the collector-emitter
voltage. The ordinate axis in each of FIGS. 39 to 41 shows the current IC as the collector
current. Accordingly, each of FIGS. 39 to 41 shows a value at which the voltage VCE
is saturated in the ON state, i.e., an ON voltage.
[0180] Also, each of FIGS. 39 to 41 shows the case where the thickness of the semiconductor
layer SLn, i.e., the thickness of the n
--type drift region ND was varied. FIG. 39 shows the case where the thickness of the
semiconductor layer SLn was set to 70 µm. FIG. 40 shows the case where the thickness
of the semiconductor layer SLn was set to 135 µm. FIG. 41 shows the case where the
thickness of the semiconductor layer SLn was set to 180 µm. Note that, in the graphs
of FIGS. 39 to 41, the display of specific numerical values is omitted and, in FIGS.
39 to 41, the abscissa axes and the ordinate axes have equal ranges.
[0181] When comparisons are made between FIGS. 39 to 41, it will be understood that the
ON voltage of the semiconductor device in Comparative Example 2 is higher than the
ON voltage of the semiconductor device in Comparative Example 1 irrespective the thickness
of the semiconductor layer SLn, i.e., the thickness of the n
--type drift region ND. Also, when comparisons are made between FIGS. 39 to 41, it
will be understood that, as the thickness of the semiconductor layer SLn, i.e., the
thickness of the n
--type drift region ND is larger, the increment in the ON voltage of the semiconductor
device in Comparative Example 2 is larger than the increment in the ON voltage of
the semiconductor device in Comparative Example 1.
[0182] FIGS. 42 to 44 are graphs each showing a hole density distribution in a thickness
direction in the semiconductor device in Comparative Example 1 in the ON state. FIGS.
45 to 47 are graphs each showing a hole density distribution in a thickness direction
in the semiconductor device in Comparative Example 2 in the ON state. FIGS. 42 to
44 show a hole density distribution in the thickness direction (Z-axis direction)
at the center position of the active cell region LCa in the X-axis direction. FIGS.
45 to 47 show a hole density distribution in the thickness direction (Z-axis direction)
at the center position of the hybrid sub-cell cell region LCh1 in the X-axis direction.
The ordinate axis in each of FIGS. 42 to 47 shows the hole density Np on a logarithmic
scale. Note that a position in the thickness direction is shown on the assumption
that a position in the thickness direction at the upper surface Sa is 0 and a direction
extending from the upper surface Sa toward the lower surface Sb is a positive direction.
[0183] FIGS. 42 and 45 show the case where the thickness of the semiconductor layer SLn
was set to 70 µm. FIGS. 43 and 46 show the case where the thickness of the semiconductor
layer SLn was set to 135 µm. FIGS. 44 and 47 show the case where the thickness of
the semiconductor layer SLn was set to 180 µm. Each of FIGS. 42 to 47 shows a hole
density distribution in the semiconductor layer SLn when the IGBT was brought into
the ON state by applying a voltage of 15 V as the voltage VGE as the gate-emitter
voltage, i.e., when the IGBT is turned ON. Note that, in the graphs of FIGS. 42 to
47, the display of specific numerical values is omitted and, in FIGS. 42 to 47, the
abscissa axes and the ordinate axes have equal ranges.
[0184] When a comparison is made between a region GA1 in the graph of FIG. 42 and a region
GA4 in the graph of FIG. 45 in each of which the thickness of the semiconductor layer
SLn was set to 70 µm, the hole density was lower in Comparative Example 2 than in
Comparative Example 1. Also, when a comparison is made between a region GA2 in the
graph of FIG. 43 and a region GA5 in the graph of FIG. 46 in each of which the thickness
of the semiconductor layer SLn was set to 135 µm, the hole density was lower in Comparative
Example 2 than in Comparative Example 1. Also, when a comparison is made between a
region GA3 in the graph of FIG. 44 and a region GA6 in the graph of FIG. 47 in each
of which the thickness of the semiconductor layer SLn was set to 180 µm, the hole
density was lower in Comparative Example 2 than in Comparative Example 1.
[0185] Therefore, it will be understood that, in the semiconductor device in Comparative
Example 2, the IE effect is lower and the hole density is lower than in the semiconductor
device in Comparative Example 1 irrespective of the thickness of the semiconductor
layer SLn, i.e., the thickness of the n
--type drift region ND. In particular, in the region of the semiconductor layer SLn
which is closer to the emitter electrode EE, i.e., the region of the semiconductor
layer SLn where the p-channel parasitic MOSFET is formed, a decrement in hole density
is larger in Comparative Example 2 than in Comparative Example 1.
[0186] This is because, when the IGBT is brought into the ON state and carriers are stored,
by the charging up of the p-type floating region PF also, the p-channel parasitic
MOSFET is brought into the ON state and holes as the carriers are discharged. Accordingly,
in the semiconductor device including the EGE-type IGBT having the p-channel parasitic
MOSFET (semiconductor device in Comparative Example 2), the IE effect is lower and
the ON voltage is higher than in the semiconductor device including the GG-type IGBT
(semiconductor device in Comparative Example 1) having no p-channel parasitic MOSFET.
[0187] In addition, as a result of a reduction in hole density as carrier density, the resistance
of the n
--type drift region ND increases to raise the ON voltage. Therefore, it can be considered
that, as the thickness of the semiconductor layer SLn, i.e., the thickness of the
n
--type drift region ND increases, the ratio of the resistance of the n
--type drift region ND to the entire resistance between the collector electrode CE
and the emitter electrode EE increases and consequently the increment in ON voltage
is larger in Comparative Example 2 than in Comparative Example 1.
[0188] Next, a description will be given of a switching loss at a turn-ON time.
[0189] FIGS. 48 and 49 are graphs each showing switching waveforms when the semiconductor
device in Comparative Example 2 is turned ON. The results shown in FIGS. 48 and 49
are obtained by calculation performed using the TCAD in accordance with the same method
as used to obtain the results shown in FIGS. 36 and 37 except that the semiconductor
device in Comparative Example 2 is not turned OFF, but is turned ON.
[0190] FIG. 48 shows the time dependences of the voltage VGE as the gate-emitter voltage,
the voltage VCE as the collector-emitter voltage, and the current IC as the collector
current in the semiconductor device in Comparative Example 2. FIG. 49 shows the time
dependences of the hole current density Jp, the hole density Np, and the potential
Vch as the potential of the channel region of the P-channel parasitic MOSFET. The
abscissa axis in each of FIGS. 48 and 49 shows the same time range.
[0191] Note that FIGS. 48 and 49 show the time dependences in the two cases where the impurity
concentration in each of the n-type hole barrier regions NHB is low and where the
impurity concentration in each of the n-type hole barrier regions NHB is high. Since
the influence of the impurity concentration in the n-type hole barrier region NHB
will be described later, a description is given here of the case where the impurity
concentration in the n-type hole barrier region NHB is low.
[0192] As shown in FIG. 35, when the voltage VGE as the switching waveform including the
first and second two pulses is applied to the semiconductor device including the IGBT,
the switching characteristic of the semiconductor device at a turn-ON time is measured
as the switching characteristic at a turn-ON time when the second pulse is applied.
[0193] As shown in FIG. 48, at the turn-ON time, as the voltage VGE rises, the voltage VCE
drops and the current IC increases. Also, as shown in FIG. 48, as the voltage VGE
rises, the voltage VCE drops, and the current IC decreases, the potential Vch rises,
the hole current density Jp increases, and the hole density Np increases. From the
foregoing, it will be understood that, when the IGBT included in the semiconductor
device is turned ON, the potential of the channel region of the p-channel parasitic
MOSFET rises to bring the parasitic MOSFET into the ON state and holes as carriers
are discharged.
[0194] On the other hand, the density distribution of holes as carriers at the turn-ON time
is the same as the density distribution of holes as carriers at the turn-OFF time
shown in FIG. 38. Accordingly, it will be understood that, from the density distribution
of holes as carriers also, holes as carries are discharged via the p-channel parasitic
MOSFET at the turn-ON time.
[0195] In the semiconductor device including the IGBT, as the IE effect increases, carriers
can be stored ahead of time at the turn-ON time. This can reduce a switching loss
at the turn-ON time. However, in the semiconductor device including the IGBT having
the EGE-type active cell region, holes as carriers are discharged via the p-channel
parasitic MOSFET at the turn-ON time. This reduces the IE effect and increases the
switching loss at the turn-ON time.
[0196] Here, as shown in FIG. 49, the hole density Np that had temporarily increased was
slow in decreasing. Accordingly, it will be understood that, after the turn-ON time,
even in the ON state, i.e., during a conduction period, holes as carriers continue
to be discharged via the p-channel parasitic MOSFET. This means that, even in the
ON state, a voltage VCEsat as the ON voltage of the IGBT included in the semiconductor
device including the IGBT rises, though to a lesser degree than at either of the turn-OFF
time and the turn-ON time, resulting in the degradation of the characteristic thereof.
[0197] As described above, the semiconductor device including the IGBT having the EGE-type
active cell region (semiconductor device in Comparative Example 2) has a problem in
that the ON voltage rises to be higher than in the semiconductor device including
the IGBT having the GG-type active cell region (semiconductor device in Comparative
Example 1) and a switching loss at the turn-ON time increases to be larger than in
the semiconductor device including the IGBT having the GG-Type active cell region.
When the ON voltage rises and the switching loss at the turn-ON time increases, a
switching loss in the inverter circuit formed of the semiconductor device increases.
Therefore, it is important to improve the disadvantage of the semiconductor device
including the IGBT having the EGE-type active cell region relative to the semiconductor
device including the IGBT having the GG-type active cell region (semiconductor device
in Comparative Example 1).
[0198] That is, in the semiconductor device including the IGBT having the EGE-type active
cell region (semiconductor device in Comparative Example 2), it is desirable to further
improve the performance of the semiconductor device such as, e.g., the IE effect.
<Main Characteristic Feature and Effect of Embodiment 1>
[0199] The semiconductor device in Embodiment 1 has the EGE-type active cell region. In
the semiconductor device in Embodiment 1, the plurality of p
+-type semiconductor regions PR are arranged along the Y-axis direction as the extending
direction of each of the trenches T1, T2, and T3 in plan view to be spaced apart from
each other.
[0200] Accordingly, in the semiconductor device in Embodiment 1, in the same manner as in
the semiconductor device having the EGE-type active cell region in Comparative Example
2, the influence of a displacement current on the potential of the gate electrode
GE can be eliminated and a switching speed when the semiconductor device in Embodiment
1 is turned OFF by the L-load switching can be improved to be higher than in the semiconductor
device having the GG-type active cell region in Comparative Example 1.
[0201] Also, in the semiconductor device in Embodiment 1, the ON voltage can be reduced
to be lower than in the semiconductor device in Comparative Example 2 in which the
p
+-type semiconductor regions PR are formed continuously along the Y-axis direction
in plan view and the switching loss when the semiconductor device in Embodiment 1
is turned ON by the L-load switching can be reduced to be smaller than in the semiconductor
device in Comparative Example 2.
[0202] That is, in the semiconductor device in Embodiment 1, the performance of the semiconductor
device such as, e.g., the IE effect can be improved to be higher than in the semiconductor
device in Comparative Example 2.
[0203] In the semiconductor device in Comparative Example 2, as shown in FIG. 28, the p
+-type semiconductor regions PR are formed continuously along the Y-axis direction
at any position in the Y-axis direction. Consequently, in the semiconductor device
in Comparative Example 2, the ON resistance of the p-channel parasitic MOSFET is small
at any position in the Y-axis direction and the channel length is short. Accordingly,
a large quantity of holes are discharged as carriers via the parasitic MOSFET.
[0204] On the other hand, in the semiconductor device in Embodiment 1, as shown in FIG.
6, the plurality of p
+-type semiconductor regions PR are arranged along the Y-axis direction to be spaced
apart from each other. In the upper-layer portion of the semiconductor layer SLn,
the p
+-type semiconductor regions PR and the p-type body regions PB are alternately arranged
along the Y-axis direction. In addition, the p-type impurity concentration in each
of the p
+-type semiconductor regions PR is higher than the p-type impurity concentration in
each of the p-type body regions PB.
[0205] In the regions where the p
+-type semiconductor regions PR are not formed, the ON resistance of the p-channel
parasitic MOSFET is higher than in the regions where the p
+-type semiconductor regions PR are formed and the channel length is longer. Accordingly,
a small quantity of holes are discharged as carriers via the parasitic MOSFET. Accordingly,
in the semiconductor device in Embodiment 1, the area ratio of the inactive section
LCbi where the p
+-type semiconductor regions PR are not formed to the active section LCba where the
p
+-type semiconductor regions PR are formed can be increased to be higher than in the
semiconductor device in Comparative Example 2. This allows a reduction in the quantity
of holes discharged as carriers via the parasitic MOSFET.
[0206] Next, a detailed description will be given of the fact that, in the semiconductor
device in Embodiment 1, the ON voltage can be reduced and the switching loss when
the semiconductor device in Embodiment 1 is turned ON by the L-load switching can
be reduced.
[0207] First, a description will be given of the fact that, in the semiconductor device
in Embodiment 1, the ON voltage can be reduced.
[0208] In the semiconductor device in Embodiment 1, the plurality of p
+-type semiconductor regions PR are arranged along the Y-axis direction as the gate
width direction of the trench gate electrode TG1 to be spaced apart from each other.
It is not that the one p
+-type semiconductor region PR is formed continuously. Accordingly, in the semiconductor
device in Embodiment 1, the area of each of the p
+-type semiconductor regions PR is smaller than in the semiconductor device in Comparative
Example 2. As a result, in the semiconductor device in Embodiment 1, the quantity
of holes discharged as carries is smaller than in the semiconductor device in Comparative
Example 2 to enhance the IE effect and allow a reduction in ON voltage.
[0209] In the semiconductor device in Embodiment 1, by suppressing the operation of the
p-channel parasitic MOSFET, the ON voltage can be reduced.
[0210] FIG. 50 is a cross-sectional view showing the hole density distribution in the semiconductor
device in Comparative Example 1 in the ON state. FIG. 51 is a cross-sectional view
showing the hole density distribution in the semiconductor device in Comparative Example
2 in the ON state.
[0211] As shown in FIG. 50, in the semiconductor device including the IGBT having the GG-type
active cell region in Comparative Example 1, no p-channel parasitic MOSFET is formed.
Consequently, holes are not discharged as carriers via the parasitic MOSFET.
[0212] On the other hand, in the semiconductor device including the IGBT having the EGE-type
active cell region in Comparative Example 2, the p-channel parasitic MOSFET is formed.
Accordingly, after the IGBT is turned ON, holes as carriers are stored to charge up
the p-type floating region PF and thus bring the p-channel parasitic MOSFET into the
ON state and a current path along which the holes are discharged as carriers via the
parasitic MOSFET is generated. As shown in FIG. 51, when the IGBT having the EGE-type
active cell region is in the ON state, the holes as carriers are discharged from the
p-channel parasitic MOSFET.
[0213] In the hole density distribution shown in FIG. 51, the hole densities are higher
in the respective portions of the p-type floating regions PF, the n-type hole barrier
regions NHB, and the p-type body regions PB which are closer to the trenches T2 and
T3 and lower in the respective portions of the p-type floating regions PF, the n-type
hole barrier regions NHB, and the p-type body regions PB which are further away from
the trenches T2 and T3, except in the p
+-type semiconductor regions PR where the hole densities are originally high.
[0214] Consequently, in Comparative Example 2 shown in FIG. 51, a hole current flows through
each of the current paths PT1 each extending from the n
--type drift region ND through the p-type floating region PF and also through the respective
portions of the p-type floating region PF, the n-type hole barrier region NHB, and
the p-type body region PB which are closer to the trenches T2 and T3. Also, in Comparative
Example 2 shown in FIG. 51, a hole current flows through each of the current paths
PT2 each extending from the n
--type drift region ND through the n-type hole barrier region NHB and also through
the respective portions of the n-type hole barrier region NHB and the p-type body
region PB which are closer to the trenches T2 and T3.
[0215] However, in Embodiment 1, the plurality of p
+-type semiconductor regions PR are arranged along the Y-axis direction as the gate
width direction of the trench gate electrode TG1 to be spaced apart from each other
and are not formed continuously along the Y-axis direction. Accordingly, in the semiconductor
device in Embodiment 1, in the portion where the p
+-type semiconductor regions PR are not formed, the operation of the p-channel parasitic
MOSFET can more reliably be suppressed than in the semiconductor device in Comparative
Example 2. This enhances the IE effect and allows a reduction in ON voltage.
[0216] Next, a description will be given of the fact that the switching loss can be reduced
when the semiconductor device in Embodiment 1 is turned ON by the L-load switching.
As described above, by suppressing the operation of the p-channel parasitic MOSFET,
the IE effect is enhanced to allow carriers to be stored ahead of time at the turn-ON
time. This can reduce the switching loss at the turn-ON time.
[0217] In the semiconductor device in Embodiment 1, when the operation of the p-channel
parasitic MOSFET is suppressed, the IE effect is enhanced to increase the absolute
quantity of carriers as a whole. Consequently, by merely calculating the relationship
between the hole current density in the channel region and dependence on the potential
of the channel region in the p-channel parasitic MOSFET, it is difficult to precisely
evaluate the IE effect in the semiconductor device in Embodiment 1. This is because,
in the semiconductor device in Embodiment 1, when the IE effect is enhanced, the quantity
of carriers stored in the n
--type drift region ND increases to increase the amount of charging up of the p-type
floating region PF, increase the potential of the channel region of the p-channel
parasitic MOSFET, and increase the quantity of holes discharged as carriers.
[0218] Accordingly, to precisely evaluate the IE effect in the semiconductor device in Embodiment
1, it is desirable to estimate a threshold voltage Vth of the p-channel parasitic
MOSFET. In addition, since the channel region of the p-channel parasitic MOSFET is
the n-type hole barrier region NHB, by increasing the impurity concentration in the
n-type hole barrier region NHB, it is possible to increase the threshold voltage Vth
of the p-channel parasitic MOSFET.
[0219] Accordingly, the following will make a comparison between the switching waveform
at the turn-OFF time and the switching waveform at the turn-ON time which have been
calculated for the semiconductor device in Comparative Example 2 using the TCAD in
each of the cases where the impurity concentration in each of the n-type hole barrier
regions NHB is low and where the impurity concentration in each of the n-type hole
barrier regions NHB is high. FIGS. 36, 37, 48, and 49 collectively show the cases
where the impurity concentration in the hole barrier layer is low and where the impurity
concentration in the hole barrier layer is high.
[0220] FIGS. 52 and 53 show the potential dependences of the hole current densities at the
turn-OFF time which have been determined from the results of calculation obtained
in FIGS. 36, 37, 48, and 49. FIG. 52 is a graph showing the potential dependence of
the hole current density when the semiconductor device in Comparative Example 2 is
turned OFF. FIG. 53 is a graph showing the potential dependence of the hole current
density when the semiconductor device in Comparative Example 2 is turned ON. In FIGS.
52 and 53, each of the hole current densities is the hole current density Jp in the
channel region of the p-channel parasitic MOSFET and each of the potentials is the
potential Vch as the potential of the channel region of the p-channel parasitic MOSFET.
[0221] As shown in FIGS. 52 and 53, in the semiconductor device in Comparative Example 2,
by increasing the impurity concentration in each of the n-type hole barrier regions
NHB, it is possible to raise the threshold voltage Vth of the p-channel parasitic
MOSFET. The semiconductor device in Embodiment 1 is similar to the semiconductor device
in Comparative Example 2 in having the EGE-type active cell region. Accordingly, by
increasing the impurity concentration in each of the n-type hole barrier regions NHB,
it is possible to raise the threshold voltage Vth of the p-channel parasitic MOSFET.
[0222] Specifically, a channel concentration as a parameter which affects the threshold
voltage Vth of the p-channel parasitic MOSFET can be adjusted by adjusting the impurity
concentration in the n-type hole barrier region NHB. Also, a channel length as another
parameter which affects the threshold voltage Vth of the p-channel parasitic MOSFET
can be adjusted by adjusting the depths of the trenches T1, T2, and T3 and the like.
[0223] Note that, in Embodiment 1, the conductivity type in each of the semiconductor regions
may also be simultaneously changed to the opposite conductivity type (the same applies
also to the following embodiments).
(Embodiment 2)
[0224] In Embodiment 2, a description will be given of an example in which a semiconductor
device is a module having a plurality of semiconductor chips each including an IGBT
having an EGE-type active cell region and the plurality of semiconductor chips are
coupled in parallel to each other.
[0225] FIG. 54 is a circuit block diagram showing an example of an electronic system using
the semiconductor device in Embodiment 2. FIG. 55 is an equivalent circuit diagram
showing the module as the semiconductor device in Embodiment 2. FIG. 55 shows two
IGBT modules 10 corresponding to a U-phase PH1 which are among six IGBT modules 10
included in an inverter INV shown in FIG. 54.
[0226] As shown in FIG. 54, the electronic system using the semiconductor device in Embodiment
2 includes a load such as a motor MOT, the inverter INV, a control circuit CTC1, and
a control circuit CTC2. Such an electronic system is, e.g., a solar power generation
system or a wind force power generation system. As the motor MOT, a 3-phase motor
is used herein. The 3-phase motor is configured so as to be driven with voltages in
three different phases. The control circuit CTC1 includes a plurality of power modules
PM1 and PM2.
[0227] In the electronic system shown in FIG. 54, an output of a power generation module
(the depiction thereof is omitted) in, e.g., the solar power generation system or
wind force power generation system is coupled to input terminals TM1 and TM2 of the
inverter INV. The dc voltage, i.e., dc power of the power generation module is supplied
to the inverter INV.
[0228] The control circuit CTC1 is configured of, e.g., an ECU (Electronic Control Unit)
and has an embedded control semiconductor chip such as an MCU (Micro Controller Unit).
The control circuit CTC1 includes the plurality of power modules PM1 and PM2. Each
of the power modules PM1 and PM2 is configured of, e.g., an ECU and has an embedded
control semiconductor chip such as an MCU.
[0229] The plurality of power modules PM1 and PM2 included in the control circuit CTC1 are
coupled to the control circuit CTC2. The inverter INV is controlled by the control
circuit CTC2. The control circuit CTC2 includes, e.g., a gate driver and a photocoupler,
though the depiction thereof is omitted. The gate driver (the depiction thereof is
omitted) included in the control circuit CTC2 is coupled to the inverter INV. At this
time, the gate driver (the depiction thereof is omitted) included in the control circuit
CTC2 is coupled to the gate electrode of the IGBT included in the inverter INV.
[0230] To the inverter INV, the motor MOT is coupled. The dc voltage, i.e., dc power supplied
from, e.g., the power module (the depiction thereof is omitted) in the solar power
generation system or wind force power generation system is converted to an ac voltage,
i.e., ac power in the inverter INV and supplied to the motor MOT. The motor MOT is
driven with the ac voltage, i.e., ac power supplied from the inverter INV.
[0231] In the example shown in FIG. 54, the motor MOT is the three-phase motor including
the U-phase PH1, a V-phase PH2, and a W-phase PH3. Accordingly, the inverter INV also
corresponds to three phases including the U-phase PH1, the V-phase PH2, and the W-phase
Ph3. The inverter INV corresponding to such three phases has the total of six pairs
of the IGBT modules 10 and diode modules 11.
[0232] The semiconductor device in Embodiment 2 is equivalent to the IGBT module 10. The
IGBT module 10 includes a plurality of IGBT chips 12. Each of the IGBT chips 12 is
equivalent to the semiconductor chip CHP (see FIG. 1).
[0233] Each of the plurality of IGBT chips 12 included in the IGBT module 10 includes the
semiconductor substrate SS, the semiconductor layer SLn, the semiconductor layer SLp,
the trenches T1, T2, and T3, the gate insulating film GI, and the trench gate electrodes
TG1, TG2, and TG3, similarly to the semiconductor device in Comparative Example 2
shown in FIGS. 26 to 28. Also, each of the plurality of IGBT chips 12 included in
the IGBT module 10 includes the p-type body region PB, the n
+-type emitter regions NE, the p-type floating region PF, the p
+-type semiconductor regions PR, the emitter electrode EE, the collector electrode
CE, and the gate electrode GE, similarly to the semiconductor device in Comparative
Example 2 shown in FIGS. 26 to 28. The p
+-type semiconductor regions PR are formed continuously along the Y-axis direction
as the extending direction of the trench T1.
[0234] Note that, when the motor MOT is a 2-phase motor, the inverter INV has the total
of four pairs of the IGBT modules 10 and the diode modules 11.
[0235] Of the inverter INV, the part located between the input potential of the motor MOT
and the power supply potential VCC is referred to as a HIGH-side part and the part
located between the input potential of the motor MOT and the ground potential GNT
is referred to as a LOW-side part. In the example shown in FIG. 54, as the HIGH-side
IGBT modules 10, three of the IGBT modules 10 are used and, as the LOW-side IGBT modules
10, three of the IGBT modules 10 are used. Also, as the HIGH-side diode modules 11,
three of the diode modules 11 are used and, as the LOW-side diode modules 11, three
of the diode modules 11 are used.
[0236] Of the two IGBT modules 10 shown in an area AR4 in FIG. 54 and corresponding to,
e.g., the U-phase, a HIGH-side IGBT module 10H includes the plurality of, e.g., six
IGBT chips 12 each made of the semiconductor chip CHP. On the other hand, of the two
IGBT modules 10 corresponding to, e.g., the U-phase, a LOW-side IGBT module 10L includes
the plurality of, e.g., six IGBT chips 12 each made of the semiconductor chip CHP.
In either of the HIGH-side part and the LOW-side part, the respective emitter electrodes
EE of the plurality of IGBT chips 12 are electrically coupled to each other and the
respective collector electrodes CE of the plurality of IGBT chips 12 are electrically
coupled to each other.
[0237] In the semiconductor device in Embodiment 2, the IGBT included in each of the semiconductor
chips CHP may also be the same as the IGBT included in the semiconductor device in
Comparative Example 2 described using FIGS. 26 to 28. According, the following will
describe the case where the IGBT included in the semiconductor chip CHP is the same
as the IGBT included in the semiconductor device in Comparative Example 2 described
using FIGS. 26 to 28.
[0238] In the example shown in FIG. 54, in each of the three phases including the U-phase
PH1, the V-phase PH2, and the W-phase PH3, between the power supply potential VCC
supplied to the inverter INV via the input terminals TM1 and TM2 and the input potential
of the motor MOT, i.e., in the HIGH-side part, the IGBT module 10 and the diode module
11 are coupled in antiparallel to each other. On the other hand, in each of the three
phases including the U-phase PH1, the V-phase PH2, and the W-phase PH3, between the
input potential of the motor MOT and the ground potential GND, i.e., in the LOW-side
part, the IGBT module 10 and the diode module 11 are coupled in antiparallel to each
other.
[0239] To each of the gate electrodes of the plurality of IGBT chips 12 included in each
of the six IGBT modules 10, the control circuit CTC2 is coupled to control each of
the plurality of IGBT chips 12 included in the six IGBT modules 10. Note that, in
each of the six diode modules 11, a plurality of diodes 13 are included and each of
the IGBT chips 12 and each of the diodes 13 are coupled in antiparallel to each other.
[0240] The current flowing in each of the IGBT modules 10 is controlled using the control
circuit CTC2 to drive and rotate the motor MOT. That is, by controlling the turning
ON/OFF of each of the IGBT modules 10 using the control circuit CTC2, the motor MOT
can be driven. When the motor MOT is thus driven, it is necessary to turn ON/OFF the
IGBT module 10, but the motor MOT includes an inductance. Accordingly, when the IGBT
module 10 is turned OFF, due to the inductance included in the motor MOT, a reverse
current in a direction reverse to the direction in which the current flows in the
IGBT module 10 is generated. Since the IGBT module 10 does not have the function of
allowing the reverse current to flow therein, by providing the diode module 11 in
antiparallel to the IGBT module 10, the reverse current is caused to flow back to
release the energy stored in the inductance.
<Semiconductor Device in Comparative Example 3>
[0241] Next, a description will be given of a semiconductor device in Comparative Example
3. The semiconductor device in Comparative Example 3 is a module including a plurality
of semiconductor chips each including an IGBT having a GG-type active cell region.
The plurality of semiconductor chips are coupled in parallel to each other.
[0242] An electronic system using the semiconductor device in Comparative Example 3 also
includes a load such as the motor MOT, the inverter INV, the control circuit CTC1,
and the control circuit CTC2, similarly to the electronic system (see FIG. 54) using
the semiconductor device in Embodiment 2. The inverter INV has the total of six pairs
of the IGBT modules 10 and the diode modules 11. The semiconductor device in Comparative
Example 3 is equivalent to the IGBT module 10.
[0243] In the semiconductor device in Comparative Example 3 also, in the same manner as
in the semiconductor device in Embodiment 2 (see FIGS. 54 and 55), the HIGH-side IGBT
module 10H includes the six IGBT chips 12 each made of the semiconductor chip CHP
and the LOW-side IGBT module 10L includes the six IGBT chips 12 each made of the semiconductor
chip CHP.
[0244] On the other hand, in the semiconductor device in Comparative Example 3, unlike in
the semiconductor device in Embodiment 2, the IGBT included in each of the semiconductor
chips CHP is an IGBT having a GG-type active cell region, i.e., the IGBT included
in the semiconductor device in Comparative Example 1 described using FIG. 25.
<Problem of Semiconductor Device in Comparative Example 3 and Main Characteristic
Feature and Effect of Embodiment 2>
[0245] Next, a description will be given of the problem of the semiconductor device in Comparative
Example 3 and the main characteristic feature and effect of Embodiment 2.
[0246] In the module as the semiconductor device in Comparative Example 3, the plurality
of IGBT chips 12 each having the GG-type active cell region are coupled in parallel
to each other. A consideration will be given of the case where, when such a module
as the semiconductor device in Comparative Example 3 operates, a difference is produced
between the positions where the individual IGBT chips are placed in a circuit or between
the electric characteristics of the individual IGBT chips. In such a case, fluctuations
may occur in the output of the module or a current may be concentrated on any of the
IGBT chips 12 to cause the breakage thereof.
[0247] For example, a consideration will be given of the case where, a difference is produced
between the floating inductances generated from circuit wires in the individual IGBT
chips, between the electric characteristics such as the threshold voltages Vth of
the individual IGBT chips, or between capacitances related to the gate electrodes,
i.e., gate capacitances in the individual IGBT chips. In such a case, when hard switching
such as L-load switching is performed, it may be possible that a gap is formed between
ON/OFF timings for the individual IGBT chips and the individual IGBT chips 12 do not
uniformly operate. Due to such imbalanced operations, fluctuations may occur in the
output of the IGBT module 10 or a current may be concentrated on any of the IGBT chips
12 to cause the breakage thereof.
[0248] Specifically, when the plurality of IGBT chips 12 included in the IGBT module 10
used in the inverter INV in, e.g., the wind force power generation system are turned
OFF, due to such imbalanced operations, fluctuations may occur in the output of the
IGBT module 10 or a current may be concentrated on any of the IGBT chips 12 to cause
the breakage thereof.
[0249] When the plurality of IGBT chips 12 coupled in parallel to each other thus operate
in the IGBT module 10, it is desirable that the individual IGBT chips 12 uniformly
operate. However, it is actually difficult to uniformly operate the individual IGBT
chips 12. For example, in the case where the IGBT chips 12 are used in the inverters
INV which are among power conversion devices, when the respective output terminals
of the inverters INV are short-circuited, it is desirable that each of the IGBT chips
12 is not broken during the period between the sensing of the occurrence of, e.g.,
an overcurrent or the like and the cutoff thereof. However, in an actual situation,
when the plurality of IGBT chips 12 coupled in parallel to each other do not uniformly
operate, fluctuations may occur in the output of the IGBT module 10 or a current may
be concentrated on any of the IGBT chips 12 to cause the breakage thereof.
[0250] In the IGBT module 10 as Comparative Example 3, to uniformly operate the plurality
of IGBT chips 12, it is desirable to ensure uniformity to each of conditions which
are the positions where the individual IGBT chips are placed in a circuit, coupling
structures to the control circuit CTC2 which controls the gate electrodes of the individual
IGBT chips 12, currents in the individual IGBT chips 12, the stabilities of switching
operations with respect to the individual IGBT chips 12, and temperatures during the
operations of the individual IGBT chips 12. To achieve this, it is necessary to design
each of the IGBT chips 12 such that the individual IGBT chips 12 uniformly operate
or arrange the individual IGBT chips 12 such that the individual IGBT chips 12 uniformly
operate. However, it is difficult to design the IGBT chips 12 such that the individual
IGBT chips 12 operate completely uniformly and arrange the IGBT chips 12 such that
the individual IGBT chips 12 operate completely uniformly. The difficulty increases
as the capacitance of each of the IGBT chips 12 increases, i.e., as the two-dimensional
area of the IGBT chip 12 increases.
[0251] In Comparative Example 3, it is also necessary to uniformly operate the large number
of active cell regions LCa (see FIG. 25) located in the IGBT chips 12. However, it
is impossible to completely uniformly operate the individual active cell regions LCa.
Accordingly, even when there is a certain degree of nonuniformity between the operations
of the individual IGBT chips 12, it is also necessary to prevent the IGBT module 10
from being broken.
[0252] As the breakdown voltage of each of the IGBT chips 12 is higher, the ON voltage of
the IGBT chip 12 rises. Accordingly, to enhance the IE effect, the p-type floating
regions PR are provided on both sides of each of the active cell regions LCa. However,
as a result of the charging up of the p-type floating regions PF or fluctuations in
a collector potential in an L-load switching operation, a displacement current flows
(in a positive (forward)/negative (backward) direction) into the gate electrode GE
via the p-type floating region PF to thus fluctuate a gate potential. Then, when the
IGBT module having the plurality of IGBT chips coupled in parallel to each other operates,
the individual IGBT modules do not uniformly operate. Here, when the displacement
current is a displacement current I, the collector potential is a collector potential
VC, a time is a time t, and a capacitance is a capacitance C0, the displacement current
I is given by the following expression (1).
[0253] On the other hand, even when the p-type floating regions PF are not provided on both
sides of each of the active cell regions LCa, a displacement current flows into the
gate electrode GE via a feedback capacitance made of the capacitance Cgd (see FIGS.
29 and 30). Accordingly, the capacitance Cgd needs to be reduced.
[0254] FIG. 56 is a graph showing the gate charge quantity dependence of a gate-emitter
voltage in the semiconductor device in Comparative Example 3. FIG. 57 is a graph showing
the gate charge quantity dependence of a gate-emitter voltage in the semiconductor
device in Embodiment 2. The abscissa axis in each of FIGS. 56 and 57 shows a charge
quantity Qg per unit area. The ordinate axis in each of FIGS. 56 and 57 shows the
voltage VGE as the gate-emitter voltage. FIGS. 56 and 57 show measured data. Note
that, in the graphs of FIGS. 56 and 57, the display of specific numerical values is
omitted and, in FIGS. 56 to 57, the abscissa axes and the ordinate axes have equal
ranges.
[0255] In the semiconductor device in Comparative Example 3 having the GG-type active cell
region, the displacement current flows into the gate electrode GE to abruptly raise
the voltage VGE at the turn-ON time and increase, e.g., the time rate of change of
the voltage VGE or the time rate of change of the current flowing in the active cell
region LCa. Consequently, noise is likely to occur in the voltage VGE. The occurrence
of the noise also causes non-uniform operations of the individual IGBT chips 12. Accordingly,
as shown in a region GA7 in FIG. 56, in the semiconductor device having the GG-type
active cell region in Comparative Example 3, the voltage VGE as the gate-emitter voltage
fluctuates.
[0256] Also, in the semiconductor device in Comparative Example 3, the amount of the displacement
current flowing into the gate electrode GE cannot be controlled by adjusting the resistance
Rg (see FIG. 30) as a gate resistance externally coupled to the control circuit CTC2
of each of the IGBT chips 12.
[0257] On the other hand, in the semiconductor device having the EGE-type active cell region
in Embodiment 2, it is possible to prevent the displacement current from flowing into
the gate electrode GE. Consequently, noise is less likely to occur in the voltage
VGE. Accordingly, as shown in FIG. 57, in the semiconductor device having the EGE-type
active cell region in Embodiment 2, the voltage VGE as the gate-emitter voltage does
not fluctuate.
[0258] FIGS. 58 and 59 are graphs showing switching waveforms when the semiconductor device
in Comparative Example 3 and the semiconductor device in Embodiment 2 are turned OFF
by the L-load switching. The abscissa axis in each of FIGS. 58 and 59 shows a time.
The ordinate axis in FIG. 58 shows the voltage VCE as a collector-emitter voltage.
The ordinate axis in FIG. 59 shows the current IC as a collector-emitter current.
FIGS. 58 and 59 show measured data. Note that, in the graphs of FIGS. 56 and 57, the
display of specific numerical values is omitted but, in FIGS. 58 and 59, the abscissa
axes and the ordinate axes have equal ranges. FIGS 58 and 59 also show the voltages
VGE as gate-emitter voltages in Comparative Example 3 and Embodiment 2.
[0259] In the semiconductor device in Comparative Example 3, under the influence of the
displacement current flowing into the gate electrode GE, when the semiconductor device
in Comparative Example 3 is turned OFF by the L-load switching, even after the quantity
of charges in the capacitance Cgd is discharged therefrom, the gate potential may
be held constant. Due to the different positions where the individual IGBT chips 12
are placed in the circuit and, e.g., the different parasitic floating inductances
of the individual IGBT chips 12, the displacement current tends to be different from
one IGBT chip to another. Also, due to the different gate potentials of the individual
IGBT chips 12 which are represented by the sums of the resistances Rg as the gate
resistances and the displacement currents, the displacement current tends to be different
from one IGBT chip to another. In such a case, when the plurality of IGBT chips electrically
coupled in parallel to each other are operated, it is difficult to uniformly operate
the individual IGBT chips 12.
[0260] The displacement current and the gate potential also tend to be different among the
plurality of active cell regions LCa (see FIG. 25) electrically coupled in parallel
to each other in the same IGBT chip 12. In such a case, when the plurality of IGBT
chips 12 electrically coupled in parallel to each other are operated, it is more difficult
to uniformly operate the individual IGBT chips 12.
[0261] On the other hand, in the semiconductor device in Embodiment 2, it is possible to
prevent the displacement current from flowing into the gate electrode GE and eliminate
the influence exerted by the displacement current on the operation of each of the
IGBT chips 12. Consequently, when the plurality of IGBT chips 12 electrically coupled
in parallel to each other are operated, it is possible to uniformly operate the individual
IGBT chips 12.
[0262] In the semiconductor device in Comparative Example 3, the capacitance of each of
the IGBT chips 12 is large so that a switching operation with respect to the signal
supplied to the gate electrode GE becomes slow. This increases the influence of the
positions at which the individual IGBT chips 12 are placed in the circuit such as,
e.g., the inductances of wires so that the individual IGBT chips 12 are less likely
to operate uniformly. As the capacitance of each of the IGBT chips 12 increases, the
time required for the switching operation increases to increase the time required
by each of the IGBT chips 12 to generate heat. As a result, the individual IGBT chips
12 are likely to generate different amounts of heat or have different temperatures.
[0263] When the individual IGBT chips 12 generate different amounts of heat or have different
temperatures, the individual IGBT chips 12 have different ON voltages or the different
threshold voltages Vth. Consequently, a current may flow in a concentrated manner
in any of the plurality of IGBT chips 12 to cause fluctuations in the voltage VGE
as the gate-emitter voltage or the breakage of the IGBT chip. Even though a characteristic
fluctuates at the same rate from one of the manufactured IGBT chips 12 to another,
when the capacitances of the IGBT chip 12 are large, the amount of fluctuation of
the characteristic from one IGBT chip to another increases to increase the amount
of fluctuation of the capacitance from one IGBT chip to another as compared with the
case where the capacitance of the IGBT chip is small.
[0264] The IGBT chips included in the semiconductor device in Comparative Example 3 are
for use in a high power conversion device so that the capacitances thereof are large.
Accordingly, the capacitance fluctuates in a large amount from one IGBT chip to another.
[0265] On the other hand, the module as the semiconductor device in Embodiment 2 includes
the plurality of IGBT chips 12 having the EGE-type active cell regions and coupled
in parallel to each other. The IGBT chips 12 provided in the semiconductor device
in Embodiment 2 are also for use in a high power conversion device, similarly to the
IGBT chips 12 included in the semiconductor device in Comparative Example 3. However,
in the semiconductor device in Embodiment 2, the capacitances of the IGBT chips 12
can be reduced to be smaller than in the semiconductor device in Comparative Example
3.
[0266] Consequently, when the plurality of IGBT chips 12 electrically coupled in parallel
to each other are operated, it is possible to reduce the influence of the positions
at which the individual IGBT chips 12 are located in the circuit and uniformly operate
the individual IGBT chips 12. In addition, it is possible to allow each of the IGBT
chips 12 to generate the same amount of heat or have the same temperature, prevent
or inhibit the voltage VGE as the gate-emitter voltage from fluctuating, and prevent
or inhibit the IGBT chips 12 from being broken. That is, it is possible to prevent
or inhibit the output of the module from fluctuating or prevent or inhibit a current
from being concentrated on any of the IGBT chips 12 to cause the breakage thereof.
Accordingly, the performance of the semiconductor device in Embodiment 2 can be improved
to be higher than that of the semiconductor device in Comparative Example 3.
[0267] Preferably, it is desirable to minimize the capacitance of each of the IGBT chips
12. For example, it is desirable that the quantity of gate charges per unit area (Qg)
which is required to raise the IGBT chip 12 until the IGBT chip 12 is turned ON is
not more than 600 nC/cm
2 or an input capacitance (Cies) per unit area is not more than 110 pF/mm
2. As a result, in the case of using the semiconductor device in Embodiment 2 as the
IGBT module 10 including the plurality of IGBT chips 12 electrically coupled in parallel
to each other, when a switching operation is performed, it is possible to allow each
of the IGBT chips 12 to generate the same amount of heat or have the same temperature.
Therefore, it is possible to prevent or inhibit the voltage VGE as the gate-emitter
voltage from fluctuating and prevent or inhibit the IGBT chips 12 from being broken.
[0268] An RBSOA (Reverse Bias Safe Operating Area) resistance when the plurality of IGBT
chips coupled in parallel to each other are operated is lower than an RBSOA resistance
when one of the IGBT chips is operated. This may be considerably because, when the
plurality of IGBT chips 12 coupled in parallel to each other are operated, if any
of the IGBT chips 12 shows a slight sign of not performing a uniform operation, a
current flows in a concentrated manner in the IGBT chip 12. Therefore, it is desirable
to improve the RBSOA resistance of each of the IGBT chips.
[0269] In the semiconductor device in Embodiment 2, in the hybrid cell region LCh as the
active cell region included in the IGBT chip 12, holes can be discharged via the p-channel
parasitic MOSFET. This can easily improve the RBSOA resistance. In addition, it is
also possible to prevent or inhibit a current from flowing in a concentrated manner
in any of the plurality of hybrid cell regions LCh included in the IGBT chip 12 such
as located in, e.g., the outermost peripheral portion of the IGBT chip 12. Thus, it
is possible to uniformly operate the hybrid cell regions LCh as the plurality of active
cell regions included in the IGBT chip 12 and coupled in parallel to each other.
[0270] The three IGBT chips 12 in each of Comparative Example 3 and Embodiment 2 were subjected
to a load short circuit test. At this time, gate potentials, collector potentials,
and collector currents were determined by performing circuit simulation using a SPICE
(Simulation Program with Integrated Circuit Emphasis), the result of which is shown
herein.
[0271] FIG. 60 is an equivalent circuit diagram showing a pseudo device model of each of
the IGBT chips included in the semiconductor device in Comparative Example 3. FIG.
61 is an equivalent circuit diagram showing a pseudo device model of each of the IGBT
chips included in the semiconductor device in Embodiment 2. FIG. 62 is a circuit diagram
for circuit simulation in each of the semiconductor devices in Comparative Example
3 and Embodiment 2. FIG. 63 is a graph showing the result of the circuit simulation
in the semiconductor device in Comparative Example 3. FIG. 64 is a graph showing the
result of the circuit simulation in the semiconductor device in Embodiment 2. Note
that, in the graphs of FIGS. 63 and 64, the display of specific numerical values is
omitted and, in FIGS. 63 to 64, the abscissa axes and the ordinate axes have equal
ranges.
[0272] In the circuit for circuit simulation shown in FIG. 62, a dc power supply BAT having
the power supply potential VCC, the capacitor CAP, and the three IGBT chips 12 are
coupled in parallel to each other. In each of the IGBT chips 12, between the collector
electrode CE and the power supply potential VCC, a floating inductor having an inductance
Lc is coupled and, between the emitter electrode EE and the ground potential, a floating
inductor having an inductance Le is coupled. In each of the IGBT chips 12, to the
gate electrode GE, an ac signal source AS is coupled via a floating inductor having
an inductance Lg and the resistance Rg.
[0273] In the load short circuit test, it is desirable to reduce the influence exerted on
the gate potential, i.e., the voltage VGE as the gate-emitter voltage. However, in
the semiconductor device in Comparative Example 3 having the GG-type active cell region,
under hard switching conditions such that the voltage of the dc power supply BAT is
directly cut off or applied, the time rate of change of a collector potential, i.e.,
the voltage VCE as the collector-emitter voltage increases upon L-load (or no-load)
switching to increase the displacement current generated in the gate electrode GE.
For example, when the voltage VCE is several thousands of volts or the current IC
as a collector current is several thousands of amperes, fluctuations in collector
potential or fluctuations in collector current significantly affect the gate potential.
[0274] In the semiconductor device in Comparative Example 3 including the IGBT chips each
having the GG-type active cell region, as shown in FIG. 25, the p-type floating region
PF and each of the trench gate electrodes TG1 and TG2 coupled to the gate electrode
GE (see FIG. 1) are adjacent to each other via the gate insulating film GI. Consequently,
as shown in FIG. 60, the displacement current path PA100 is coupled to the gate electrode
GE. Accordingly, as shown in FIG. 63, the gate potential (voltage VGE), the collector
potential (voltage VCE), and the collector current (current IC) fluctuate.
[0275] On the other hand, in the semiconductor device in Embodiment 2 including the IGBT
chips each having the EGE-type active cell region, as shown in FIG. 4, the p-type
floating region PF and the trench gate electrode TG1 coupled to the gate electrode
GE are cut off by each of the trench gate electrodes TG2 and TG3 coupled to the emitter
electrode EE and are not adjacent to each other. Consequently, as shown in FIG. 61,
the displacement current flows along a displacement current path PA1 coupled to the
emitter electrode EE, but the displacement current scarcely flows along a displacement
current path PA2 coupled to the gate electrode GE. Accordingly, as shown in FIG. 64,
the gate potential (voltage VGE), the collector potential (voltage VCE), and the collector
current (current IC) do not fluctuate.
[0276] That is, in the semiconductor device in Embodiment 2, it is possible to prevent the
displacement current from flowing into the gate electrode GE. Accordingly, in the
load short circuit test, even under hard switching conditions, it is possible to prevent
the displacement current from affecting the gate potential.
<Modification of Semiconductor Device in Embodiment 2>
[0277] Each of the IGBT chips included in the semiconductor device in Embodiment 2 is a
semiconductor device as an IGBT chip having an EGE-type active cell region. In each
of the hybrid cell regions LCh as the active cell region, the p
+-type semiconductor regions PR are formed continuously along the Y-axis direction.
Since it is sufficient for each of the IGBT chips included in the semiconductor device
in Embodiment 2 to be a semiconductor device as the IGBT chip having the EGE-type
active cell region, in each of the hybrid cell regions LCh as the active cell region,
a plurality of the p
+-type semiconductor regions PR may also be arranged along the Y-axis direction to
be spaced apart from each other. Such an example will be described as a modification
of the semiconductor device in Embodiment 2.
[0278] In each of the IGBT chips included in the semiconductor device in the present modification,
in the same manner as in each of the IGBT chips as the semiconductor device in Embodiment
1, the plurality of p
+-type semiconductor regions PR are arranged in the Y-axis direction to be spaced apart
from each other. In addition, in each of the hybrid sub-cell regions LCh1 and LCh2,
the plurality of n
+-type emitter regions NE are placed at the same positions as those of the p
+-type semiconductor regions PR in the Y-axis direction.
[0279] Accordingly, the semiconductor device in the present modification has the same effect
as the effect exerted by the semiconductor device in Embodiment 1 on the semiconductor
device in Comparative Example 2. In the semiconductor device in the present modification,
the ON voltage can be reduced to be lower than in the semiconductor device in Embodiment
2 and the switching loss when the semiconductor device in the present modification
is turned ON by L-load switching can be reduced to be smaller than in the semiconductor
device in Embodiment 2.
(Embodiment 3)
[0280] In Embodiment 3, a description will be given of an example in which, in a semiconductor
device including an IGBT having an EGE-type active cell region, the width of the active
cell region is small and a coupling electrode overlaps a trench gate electrode in
plan view.
[0281] In the semiconductor device in Embodiment 3, the IGBT included in the semiconductor
chip CHP (see FIG. 1) may be the same as the IGBT included in the semiconductor device
in Comparative Example 2 described using FIGS. 26 to 28. Accordingly, the following
will describe the case where the IGBT included in the semiconductor chip CHP is the
same as the IGBT included in the semiconductor device in Comparative Example 2.
<Configuration of Semiconductor Device>
[0282] First, a description will be given of a configuration of the semiconductor device
in Embodiment 3.
[0283] A structure of the semiconductor device in Embodiment 3 is the same as the structure
of the semiconductor device in Comparative Example 2 described using FIGS. 26 to 28
except that, in plan view, the coupling electrode CP overlaps the trench gate electrodes
TG2 and TG3. Accordingly, the following will mainly describe a point different from
the structure of the semiconductor device in Comparative Example 2.
[0284] FIG. 65 is a main-portion plan view of the semiconductor device in Embodiment 3.
FIG. 66 is a cross-sectional view along the line A-A in FIG. 65. Note that the cross-sectional
view along the line B-B in FIG. 65 is the same as the cross-sectional view shown in
FIG. 66 except that the n
+-type emitter regions NE are not provided.
[0285] In the semiconductor device in Embodiment 3, in the same manner as in the semiconductor
device in Comparative Example 2, the plurality of n
+-type emitter regions NE are formed in each of the hybrid sub-cell regions LCh1 and
LCh2.
[0286] Also, in Embodiment 3, in the same manner as in Comparative Example 2, in the hybrid
sub-cell region LCh1, the p
+-type semiconductor regions PR are formed continuously along the Y-axis direction
as the extending direction of each of the trenches T1, T2, and T3. Also, in the hybrid
sub-cell region LCh1, in the p-type body region PB, the contact trenches CT as openings
are formed continuously along the Y-axis direction. The contact trenches CT reach
the p
+-type body contact region PBC placed in the hybrid sub-cell region LCh1.
[0287] Also, in Embodiment 3, in the same manner as in Comparative Example 2, the p
+-type semiconductor regions PR are formed continuously along the Y-axis direction
in the hybrid sub-cell region LCh2. Also, in the hybrid sub-cell region LCH2, in the
p-type body region PB, the contact trenches CT as the openings are formed continuously
along the Y-axis direction. The contact trenches CT reach the p
+-type body contact region PBC placed in the hybrid sub-cell region LCh2.
[0288] On the other hand, in the semiconductor device in Embodiment 3, unlike in the semiconductor
device in Comparative Example 2, the contact trench CT overlaps the trench T2 in plan
view in the hybrid sub-cell region LCh1 and the contact trench CT overlaps the trench
T3 in plan view in the hybrid sub-cell region LCh2.
[0289] Alternatively, in the hybrid sub-cell region LCh2, the p
+- type semiconductor region PR may also be in contact with the gate insulating film
GI formed over the inner wall of the trench T2 and, in the hybrid sub-cell region
LCh2, the p
+-type semiconductor region PR may also be in contact with the gate insulating film
GI formed over the inner wall of the trench T3.
<Method of Manufacturing Semiconductor Device>
[0290] A method of manufacturing the semiconductor device in Embodiment 3 is the same as
the method of manufacturing the semiconductor device in Embodiment 1 described using
FIGS. 7 to 24 except that the coupling electrode CP overlaps the trench gate electrodes
TG2 and TG3 in plan view.
[0291] That is, in the manufacturing process of the semiconductor device in Embodiment 3,
the contact trench CT is formed in the hybrid sub-cell region LCh1 so as to overlap
the trench T2 in plan view, while the contact trench CT is formed in the hybrid sub-cell
region LCh2 so as to overlap the trench T3 in plan view.
[0292] Note that, in the manufacturing process of the semiconductor device in Embodiment
3, unlike in Embodiment 1, in each of the hybrid sub-cell regions LCh1 and LCh2, the
contact trenches CT are formed continuously along the Y-axis direction (see FIG. 65)
in plan view and the p
+-type semiconductor regions PR are formed continuously along the Y-axis direction
in plan view.
<About Problem of Semiconductor Device in Comparative Example 2>
[0293] To improve the performance of an IGBT, it is desirable to reduce the ON voltage and
reduce the switching loss and, to reduce the ON voltage and reduce the switching loss,
it is desirable to enhance the IE effect.
[0294] That is, in the semiconductor device (semiconductor device in Comparative Example
2) including the IGBT having the EGE-type active cell region, it is desirable to further
improve the performance of the semiconductor device such as, e.g., the IE effect.
[0295] To enhance the IE effect in the IGBT, it is effective to enhance the efficiency of
electron injection from the emitter electrode EE. Also, to enhance the efficiency
of electron injection from the emitter electrode EE, it is effective to reduce a hole
current.
[0296] Here, in the portion between the trenches T1 and T2 which extends from the bottom
portions of the trenches T1 and T2 to the p-type body region PB, the hole current
is dominated by a diffusion current. Also, in the semiconductor device in Comparative
Example 2, the portion of the semiconductor layer SLn which is located between the
trench T1 and T2 has a width in the Y-axis direction that is wider than in the semiconductor
device in Embodiment 3. Accordingly, in the semiconductor device in Comparative Example
2, it may be possible that a hole discharge resistance is lower, holes are less likely
to be stored in the portion of the n
--type drift region NE which is closer to the emitter electrode EE, the efficiency
of electron injection from the emitter electrode EE is lower, and the IE effect is
lower than in the semiconductor device in Embodiment 3. Note that what applies to
the portion between the trenches T1 and T2 similarly applies to the portion between
the trenches T1 and T3.
<Main Characteristic Feature and Effect of Embodiment 3>
[0297] On the other hand, in the semiconductor device in Embodiment 3, the coupling electrode
CP provided in the hybrid sub-cell region LCh1 overlaps the trench gate electrode
TG2 and the coupling electrode CP provided in the hybrid sub-cell region LCh2 overlaps
the trench gate electrode TG3.
[0298] In the semiconductor device in Embodiment 3, the widths of the portions of the semiconductor
layer SLn which are located between the trenches T1 and T2 and between the trenches
T1 and T3 are smaller. Accordingly, in the semiconductor device in Embodiment 3, the
hole discharge resistance is higher, holes are more likely to be stored in the portion
of the n
--type drift region ND which is closer to the emitter electrode EE, the efficiency
of electron injection from the emitter electrode EE is higher, and the IE effect is
higher than in the semiconductor device in Comparative Example 2. Therefore, the performance
of the semiconductor device in Embodiment 3 can be improved to be higher than in the
semiconductor device in Comparative Example 2.
<Modification of Semiconductor Device in Embodiment 3>
[0299] Each of the IGBT chips included in the semiconductor device in Embodiment 3 is a
semiconductor device as an IGBT chip having an EGE-type active cell region. In the
hybrid cell region LCh as each the active cell regions, the p
+-type semiconductor regions PR are formed continuously along the Y-axis direction
as the extending direction of each of the trenches T1, T2, and T3.
[0300] Since it is sufficient for each of the IGBT chips included in the semiconductor device
in Embodiment 3 to be a semiconductor device as the IGBT chip having the EGE-type
active cell region, in each of the hybrid cell regions LCh as the active cell region,
the plurality of p
+-type semiconductor regions PR may also be arranged in the Y-axis direction to be
spaced apart from each other. Such an example will be described as a modification
of the semiconductor device in Embodiment 3.
[0301] FIG. 67 is a main-portion plan view of the semiconductor device in the modification
of Embodiment 3. FIG. 68 is a main-portion cross-sectional view of the semiconductor
device in the modification of Embodiment 3. FIG. 68 is a cross-sectional view along
the line B-B in FIG. 67. Note that the cross-sectional view along the line A-A in
FIG. 67 is the same as the cross-sectional view shown in FIG. 66.
[0302] In each of the IGBT chips included in the semiconductor device in the present modification,
in the same manner as in each of the IGBT chips as the semiconductor device in Embodiment
1, the plurality of p
+-type semiconductor regions PR are arranged in the Y-axis direction to be spaced apart
from each other. Also, in the present modification, in the same manner as in Embodiment
1, in each of the hybrid sub-cell regions LCh1 and LCh2, the plurality of n
+-type emitter regions NE are placed at the same positions as those of the p
+-type semiconductor regions PR in the Y-axis direction.
[0303] Accordingly, in the present modification, in the hybrid sub-cell region LCh1, each
of the plurality of contact trenches CT overlaps the trench T2 in plan view and, in
the hybrid sub-cell region LCh2, each of the plurality of contact trenches CT overlaps
the trench T3 in plan view.
[0304] Alternatively, in the hybrid sub-cell region LCh1, each of the plurality of p
+-type semiconductor regions PR may also be in contact with the gate insulating film
GI formed over the inner wall of the trench T2 and, in the hybrid sub-cell region
LCh2, each of the plurality of p
+-type semiconductor regions PR may be in contact with the gate insulating film GI
formed over the inner wall of the trench T3.
[0305] Accordingly, the semiconductor device in the present modification has the same effect
as the effect exerted by the semiconductor device in Embodiment 1 on the semiconductor
device in Comparative Example 2. In the semiconductor device in the present modification,
the ON voltage can be reduced to be lower than in the semiconductor device in Embodiment
3 and the switching loss when the semiconductor device in the present modification
is turned ON by L-load switching can be reduced to be smaller than that in the semiconductor
device in Embodiment 3.
(Embodiment 4)
[0306] In Embodiment 4, a description will be given of an example in which a semiconductor
device includes an IGBT having an EE-type (emitter-emitter-type) inactive cell region
(non-active cell region) in addition to an EGE-type active cell region. Note that
the possession of the EE-type inactive cell region by the IGBT means that each of
two trench gate electrodes arranged in the inactive cell region to be spaced apart
from each other is electrically coupled to the emitter electrode.
[0307] In the semiconductor device in Embodiment 4, the EGE-type active cell region of the
IGBT included in the semiconductor chip CHP (see FIG. 1) may also be the same as the
EGE-type active cell region of the IGBT included in the semiconductor device in Comparative
Example 2 described using FIGS. 26 to 28. Accordingly, the following will describe
the case where the EGE-type active cell region of the IGBT included in the semiconductor
chip CHP is the same as the EGE-type active cell region of the IGBT included in the
semiconductor device in Comparative Example 2.
[0308] FIG. 69 is a main-portion plan view of the semiconductor device in Embodiment 4.
FIG. 70 is a main-portion cross-sectional view of the semiconductor device in Embodiment
4. FIG. 70 is a cross-sectional view along the line A-A in FIG. 69. Note that a cross-sectional
view along the line B-B in FIG. 69 is the same as the cross-sectional view shown in
FIG. 70 except that the n
+-type emitter regions NE are not provided.
[0309] In the semiconductor device in Embodiment 4, in the same manner as in the semiconductor
device in Comparative Example 2, each of the unit cell regions LC has the hybrid cell
region LCh as the active cell region and the two inactive cell regions LCi. Also,
in the semiconductor device in Embodiment 4, in the same manner as in the semiconductor
device in Comparative Example 2, in each of the hybrid sub-cell regions LCh1 and LCh2,
the plurality of n
+-type emitter regions NE are formed.
[0310] In Embodiment 4, in the same manner as in Comparative Example 2, in the hybrid sub-cell
region LCh1, the p
+-type semiconductor regions PR are formed continuously along the Y-axis direction
as the extending direction of each of the trenches T1, T2, and T3. Also, in the hybrid
sub-cell region LCh1, in the p-type body region PB, the contact trenches CT as an
opening are formed continuously along the Y-axis direction. The contact trenches CT
reach the p
+-type body contact region PBC located in the hybrid sub-cell region LCh1.
[0311] Also, in Embodiment 4, in the same manner as in Comparative Example 2, in the hybrid
sub-cell region LCh2, the p
+-type semiconductor regions PR are formed continuously along the Y-axis direction.
Also, in the hybrid sub-cell region LCh2, in the p-type body region PB, the contact
trenches CT as the openings are formed continuously along the Y-axis direction. The
contact trenches CT reach the p
+-type body contact region PBC located in the hybrid sub-cell region LCh2.
[0312] On the other hand, in Embodiment 4, unlike in Comparative Example 2, each of the
unit cell regions LC further has an inactive cell region LCe as the EE-type inactive
cell region and the third inactive cell region LCi. The inactive cell region LCe is
located opposite to the hybrid cell region LCh in the X-axis direction relative to
the inactive cell region LCi interposed therebetween. The third inactive cell region
LCi is located opposite to the other inactive cell regions LCi in the X-axis direction
relative to the inactive cell region LCe interposed therebetween.
[0313] Each of the inactive cell region LCe and the third inactive cell region LCi extends
in the Y-axis direction in plan view. The inactive cell region LCe has a width We
smaller than the width Wh of the hybrid cell region LCh. Preferably, the width We
of the inactive cell region LCe is smaller than the width Wi of the inactive cell
region LCi.
[0314] The two unit cell regions LC adjacent to each other in the X-axis direction share
the one inactive cell region LCi. Accordingly, each of the unit cell regions LC has
the positive half portion LCi1 of the inactive cell region LCi located on the negative
side of the hybrid cell region LCh in the X-axis direction to be adjacent thereto.
The unit cell region LC also has the negative half portion LCi2 of the inactive cell
region LCi (the third inactive cell region LCi) located on the positive side of the
inactive cell region LCe in the X-axis direction to be adjacent thereto.
[0315] The inactive cell region LCi located between the inactive cell regions LCe and LCh
is referred to as an inactive cell region LCi0. The p-type floating region PF in the
inactive cell region LCi0 is formed in the portion of the semiconductor layer SLn
which is located between the trenches T3 and T4.
[0316] The inactive cell region LCe has trench gate electrodes TG4 and TG5. The trench gate
electrode TG4 is located between the inactive cell regions LCe and LCi0. The trench
gate electrode TG5 is located between the inactive cell region LCe and the portion
LCi2 of the inactive cell region LCi. The trench gate electrodes TG4 and TG5 are electrically
coupled to the emitter electrode EE.
[0317] In the inactive cell region LCe, unlike in the hybrid cell region LCH, the n
+-type emitter regions NE are not formed.
[0318] In the third inactive cell region LCi, the p-type floating region PF is provided
in the same manner as in another of the inactive cell regions LCi. The p-type floating
region PF provided in the third inactive cell region LCi is formed in the portion
of the semiconductor layer SLn which is located opposite to the trench T4 relative
to the trench T5 interposed therebetween. Preferably, the p-type floating region PF
provided in the third inactive cell region LCi is in contact with the gate insulating
film GI formed over the inner wall of the trench T5.
[0319] The end portion of the lower surface Sb of the p-type floating region PF provided
in the third inactive cell region LCi which is closer to the lower surface Sb is located
closer to the lower surface Sb than the respective end portions of the trenches T4
and T4 respectively formed with the trench gate electrodes TG4 and TG5 which are closer
to the lower surface Sb. In such a case, even when the width Wi of the inactive cell
region LCi in the X-axis direction is larger than the width We of the inactive cell
region LCe in the X-axis direction, a sufficient breakdown voltage can be ensured.
[0320] Note that, in the example shown in FIGS. 69 and 70, the width We of the inactive
cell region LCe in the X-axis direction is set smaller than the width Wi of the inactive
cell region LCi in the X-axis direction. In such a case, the IE effect can be enhanced.
[0321] Next, a description will be given of a configuration of each of the unit cell regions
LC in the semiconductor chip as the semiconductor device in Embodiment 4.
[0322] The trench T4 is located opposite to the trench T1 relative to the trench T3 interposed
therebetween to extend in the Y-axis direction in plan view from the upper surface
Sa of the semiconductor substrate SS and reach a middle point in the semiconductor
layer SLn. Over the inner wall of the trench T4, the gate insulating film GI is formed.
In the trench T4, the trench gate electrode TG4 is formed over the gate insulating
film GI so as to be embedded in the trench T4. The trench gate electrode TG4 is electrically
coupled to the emitter electrode EE.
[0323] The trench T5 is located opposite to the trench T3 relative to the trench T4 interposed
therebetween to extend in the Y-axis direction in plan view from the upper surface
Sa of the semiconductor substrate SS and reach a middle point in the semiconductor
layer SLn. Over the inner wall of the trench T5, the gate insulating film GI is formed.
In the trench T5, the trench gate electrode TG5 is formed over the gate insulating
film GI so as to be embedded in the trench T5. The trench gate electrode TG5 is electrically
coupled to the emitter electrode EE.
[0324] In the inactive cell region LCe, the p-type body region PB is formed in the portion
of the semiconductor layer SLn which is located between the trenches T4 and T5 to
be in contact with the gate insulating film GI formed over the inner wall of the trench
T4 and with the gate insulating film GI formed over the inner wall of the trench T5.
[0325] In the inactive cell region LCe, the p
+-type semiconductor region PR including the p
+-type body contact region PBC and the p
+-type latch-up preventing region PLP is formed in the portion of the semiconductor
layer SLn which is located between the trenches T4 and T5 to be in contact with the
p-type body region PB. The p
+-type semiconductor region PR is electrically coupled to the emitter region EE. In
the inactive cell region LCe, the p-type impurity concentration in the p
+-type semiconductor region PR is higher than the p-type impurity concentration in
the p-type body region PB.
[0326] The interlayer insulating film IL is formed in the inactive cell region LCe so as
to cover the p-type body region PB. In the inactive cell region LCe, in the interlayer
insulating film IL and the semiconductor layer SLn, the contact trenches CT as openings
are formed to extend through the interlayer insulating film IL and reach a middle
point in the semiconductor layer SLn. In the inactive cell region LCe, the contact
trenches CT extend in the Y-axis direction in plan view. In the inactive cell region
LCe, the p
+-type semiconductor region PR is formed in the portion of the p-type body region PB
which is exposed in each of the contact trenches CT. In the inactive cell region LCe,
the coupling electrodes CP embedded in the contact trenches CT are formed. In the
inactive cell region LCe, each of the coupling electrodes CP is in contact with the
p
+-type semiconductor region PR. Consequently, the p
+-type semiconductor region PR formed in the inactive cell region LCe is electrically
coupled to the emitter electrode EE via the coupling electrode CP.
[0327] Note that, as described above, in the inactive cell region LCe, the n
+-type emitter regions NE are not formed. Accordingly, the inactive cell region LCe
does not operate as the IGBT.
[0328] In Embodiment 4, in the inactive cell region LCe, the n-type hole barrier region
NHB as the n-type semiconductor region is not formed under the p-type body region
PB.
<Method of Manufacturing Semiconductor Device>
[0329] A method of manufacturing the semiconductor device in Embodiment 4 is the same as
the method of manufacturing the semiconductor device in Embodiment 1 described using
FIGS. 7 to 24 in that, in addition to the hybrid cell region LCh, the inactive cell
region LCe is formed. Also, the step of forming the inactive cell region LCe can be
the same as the step of forming the hybrid sub-cell region LCh1 except that the trenches
T4 and T5 are formed similarly to the trenches T2 and T1 and the n-type hole barrier
regions NHB and the n
+-type emitter regions NE are not formed.
[0330] Note that, in the manufacturing process of the semiconductor device in Embodiment
4, unlike in Embodiment 1, the contact trench CT is formed continuously along the
Y-axis direction (see FIG. 69) in plan view in each of the hybrid sub-cell regions
LCh1 and LCh2 and the p
+-type semiconductor region PR is formed continuously along the Y-axis direction in
plan view.
<Problem of Semiconductor Device in Comparative Example 2>
[0331] To enhance the performance of an IGBT, it is desirable that the holes as carriers
stored in the n
--type drift region ND in the hybrid cell region LCh when the IGBT is in the ON state
are efficiently discharged when the semiconductor device is turned OFF by L-load switching.
[0332] That is, in the semiconductor device including the IGBT having the EGE-type active
cell region (semiconductor device in Comparative Example 2), it is desirable to further
improve the performance of the semiconductor device such as, e.g., hole discharge
efficiency when the semiconductor device is turned OFF.
[0333] In the IGBT having the hybrid cell region LCh, to efficiently discharge holes in
the hybrid cell region LCh at a turn-OFF time, it is desirable to reduce the threshold
voltage Vth of a p-channel parasitic MOSFET.
[0334] However, when the n-type hole barrier regions NHB are formed in the hybrid cell region
LCh in the semiconductor device in Comparative Example 2, the n-type impurity concentration
in each of the n-type hole barrier regions NHB is higher than the n-type impurity
concentration in the n
+-type drift region ND. Therefore, the threshold voltage Vth of the p-channel parasitic
MOSFET cannot be reduced. As a result, it is impossible to efficiently discharge the
holes as carriers stored in the n
+-type drift region ND in the hybrid cell region LCh when the IGBT is in the OFF state
and is impossible to increase the speed of a turn-OFF operation.
<Main Characteristic Feature and Effect of Embodiment 4>
[0335] In the semiconductor device in Embodiment 4, the unit cell region LC includes the
inactive cell region LCe in addition to the hybrid cell region LCh. In the hybrid
cell region LCh, the n-type hole barrier regions NHB are formed while, in the inactive
cell region LCe, the n-type hole barrier regions NHB are not formed.
[0336] Accordingly, in the semiconductor device in Embodiment 4, even when the threshold
voltage Vth of the p-channel parasitic MOSFET formed in the hybrid cell region LCh
is high due to the n-type hole barrier regions NHB, the threshold voltage Vth of the
p-channel parasitic MOSFET in the inactive cell region LCi can be reduced. Consequently,
in the inactive cell region LCe, the holes as carriers stored in the n
--type drift region ND in the hybrid cell region LCh when the IGBT is in the ON state
can efficiently be discharged when the IGBT is turned OFF. This can increase the speed
of the turn-OFF operation.
[0337] Thus, the performance of the semiconductor device in Embodiment 4 such as, e.g.,
the hole discharge efficiency at a turn-OFF time can be improved to be higher than
in the semiconductor device in Comparative Example 2.
[0338] Also, in the semiconductor device in Embodiment 4, in the hybrid cell region LCh,
the n
+-type emitter regions NE are formed and the parasitic bipolar transistor made of an
npn bipolar transistor is formed. However, in the semiconductor device in Embodiment
4, in the inactive cell region LCe, the n
+-type emitter regions NE are not formed and the parasitic bipolar transistor made
of the npn bipolar transistor is not formed. Consequently, in the semiconductor device
in Embodiment 4, in the inactive cell region LCe, a latch-up is less likely to occur.
Therefore, a breakdown resistance such as the RBSOA resistance can be improved to
be higher than in the semiconductor device in Comparative Example 2.
<Modification of Semiconductor Device in Embodiment 4>
[0339] The IGBT chip included in the semiconductor device in Embodiment 4 is a semiconductor
device as an IGBT chip having EGE-type active cell regions. In the hybrid cell region
LCh as each of the active cell regions, the p
+-type semiconductor regions PR are formed continuously along the Y-axis direction
as the extending direction of each of the trenches T1 and T2.
[0340] Since it is sufficient for the IGBT chip included in the semiconductor device in
Embodiment 4 to be a semiconductor device as the IGBT chip having the EGE-type active
cell regions, in the hybrid cell region LCh as each of the active cell regions, the
plurality of p
+-type semiconductor regions PR may be arranged in the Y-axis direction to be spaced
apart from each other. Such an example will be described as a modification of the
semiconductor device in Embodiment 4.
[0341] FIG. 71 is a main-portion plan view of the semiconductor device in the modification
of Embodiment 4. FIG. 72 is a main-portion cross-sectional view of the semiconductor
device in the modification of Embodiment 4. FIG. 72 is a cross-sectional view along
the line B-B in FIG. 71. Note that the cross-sectional view along the line A-A in
FIG. 71 is the same as the cross-sectional view shown in FIG. 70.
[0342] In the IGBT chip included in the semiconductor device in the present modification,
in the same manner as in the semiconductor device in Embodiment 1, the plurality of
p
+-type semiconductor regions PS are arranged in the Y-axis direction to be spaced apart
from each other. Also, in the present modification, in the same manner as in Embodiment
1, in each of the hybrid cell formation regions LCh1 and LCh2, the plurality of n
+-type emitter regions NE are located at the same positions in the Y-axis direction
as those of the p
+-type semiconductor regions PS.
[0343] Accordingly, the semiconductor device in the present modification has the same effect
as the effect exerted by the semiconductor device in Embodiment 1 on the semiconductor
device in Comparative Example 2. In the semiconductor device in the present modification,
the ON voltage can be reduced to be lower than in the semiconductor device in Embodiment
4 and the switching loss when the semiconductor device is turned ON by L-load switching
can be reduced to be smaller than in the semiconductor device in Embodiment 4.
[0344] While the invention achieved by the present inventors has been specifically described
heretofore on the basis of the embodiments thereof, the present invention is not limited
to the foregoing embodiments. It will be appreciated that various changes and modifications
can be made in the invention within the scope not departing from the gist thereof.